US11786754B2

US11786754B2 - Adaptive aperture

Info

Publication number: US11786754B2
Application number: US17/567,544
Authority: US
Inventors: Gerrit Townsend Zwart; Mark R. Jones; Miles S. Wagner; James Cooley; Eros Pedroni; Robert Silva
Original assignee: Mevion Medical Systems Inc
Current assignee: Mevion Medical Systems Inc
Priority date: 2015-11-10
Filing date: 2022-01-03
Publication date: 2023-10-17
Anticipated expiration: 2035-11-10
Also published as: EP3374023A1; US20210038915A1; WO2017082984A1; JP2018536522A; ES2779823T3; US11213697B2; US10646728B2; EP3374023B1; US20220118284A1; US20170128746A1; US20170157422A1; EP3698849A1; JP7091247B2; US10786689B2; CN108883295B; CN108883295A; JP2022118114A

Abstract

An example particle therapy system includes a particle accelerator to output a particle beam having a spot size; a scanning system for the particle accelerator to scan the particle beam in two dimensions across at least part of a treatment area of an irradiation target; and an adaptive aperture between the scanning system and the irradiation target. The adaptive aperture includes structures that are movable relative to the irradiation target to approximate a shape to trim part of the treatment area. The part of the treatment area has a size that is based on an area of the spot size.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of U.S. patent application Ser. No. 16/999,641 which was filed on Aug. 21, 2022; U.S. patent application Ser. No. 16/999,641 being a continuation of U.S. patent application Ser. No. 14/937,048 which was filed on Nov. 10, 2015 and which issued as U.S. Pat. No. 10,786,689 on Sep. 29, 2020. This application claims priority to U.S. patent application Ser. No. 16/999,641 and to U.S. patent application Ser. No. 14/937,048. This application also has the same specification as U.S. patent application Ser. No. 15/438,544, which is a continuation of U.S. patent application Ser. No. 14/937,048, which was filed on Feb. 21, 2017, and which issued as U.S. Pat. No. 10,646,728 on May 12, 2020. The contents of U.S. patent application Ser. Nos. 16/999,641, 14/937,048, and 15/438,544 are incorporated herein by reference.

TECHNICAL FIELD

This disclosure relates generally to an adaptive aperture for use, e.g., with a particle therapy system.

BACKGROUND

Particle therapy systems use an accelerator to generate a particle beam for treating afflictions, such as tumors. In operation, particles are accelerated in orbits inside a cavity in the presence of a magnetic field, and are removed from the cavity through an extraction channel. A magnetic field regenerator generates a magnetic field bump near the outside of the cavity to distort the pitch and angle of some orbits so that they precess towards, and eventually into, the extraction channel. A beam, comprised of the particles, exits the extraction channel.

A scanning system is down-beam of the extraction channel. In this context, “down-beam” means closer to an irradiation target (here, relative to the extraction channel). The scanning system moves the particle beam across at least part of the irradiation target to expose various parts of the irradiation target to the particle beam. For example, to treat a tumor, the particle beam may be “scanned” over different cross-sectional layers of the tumor.

The particle beam can damage healthy tissue adjacent to the irradiation target. A structure containing an aperture may be used to limit exposure of the healthy tissue to the particle beam. For example, the structure, or a portion thereof, may be placed in between the particle beam and the healthy tissue, thereby preventing exposure of the healthy tissue to the particle beam.

SUMMARY

An example particle therapy system comprises a particle accelerator to output a particle beam having a spot size; a scanning system for the particle accelerator to scan the particle beam in two dimensions across at least part of a treatment area of an irradiation target; and an adaptive aperture between the scanning system and the irradiation target. The adaptive aperture comprises structures that are movable relative to the irradiation target to approximate a shape to trim part of the treatment area. The part of the treatment area has a size that is based on an area of the spot size. The example particle therapy system may include one or more of the following features, either alone or in combination.

The size of the part of the treatment area may be about the same as the area of spot size, the area of two spot sizes, the area of three spot sizes, the area of four spot sizes, or the area of five spot sizes. The part of the treatment area may be less than an entirety of the treatment area. The structures may be movable relative to the irradiation target to approximate a shape that is at least partly curved.

The adaptive aperture may comprise a primary carriage coupled to the structures to move the structures relative to the irradiation target in a vertical dimension relative to the irradiation target; a first motor to control movement of the primary carriage; secondary carriages coupled to the primary carriage and to the structures to move the structures horizontally relative to the irradiation target; and one or more secondary motors to control movement of the structures horizontally. The horizontal movement may comprise movement into, and out of, the treatment area. The secondary carriages may comprise a first secondary carriage coupled to the primary carriage to move at least some of the structures relative to the irradiation target; and a second secondary carriage coupled to the primary carriage to move at least some of the structures relative to the irradiation target. At least one of the secondary carriages may be rotatable relative to primary carriage, and/or the entire adaptive aperture may be rotatable relative to the irradiation target.

In the particle therapy system, at least some structures movable by the first secondary carriage have flat edges and at least some structures movable by the second secondary carriage have flat edges. The first secondary carriage may be mounted on, and movable along, a track this is curved; and the second secondary carriage may be mounted on, and movable along, the track that is curved.

The structures may comprise leaves, at least some of which have widths that are different from heights of others of the leaves. The at least some of the leaves may have widths that are three or more times heights of the others of the leaves. The leaves may comprise metal, such as nickel or tungsten.

The particle therapy system may comprise memory storing instructions that are executable; and one or more processing devices to execute the instructions to configure the adaptive aperture by controlling movement of the structures.

The movement of the structures may be controlled based on operation of the scanning system. The scanning system may be controllable to scan the particle beam across the treatment area multiple times. The movement of the structures may be controllable so that, for different scans of the particle beam across at least part of the treatment area, a configuration of the structures changes. For different scans of the particle beam across the treatment area, the configuration of the structures may be shifted vertically relative to the treatment area. For different scans of the particle beam across the treatment area, the configuration of the structures may be shifted horizontally relative to the treatment area.

The structures may comprise between five and fifty leaves. The adaptive aperture may comprise a primary carriage to which the leaves are connected to move the leaves relative to the irradiation target in a vertical dimension relative to the irradiation target; a first motor to control movement of the primary carriage; a first secondary carriage coupled to the primary carriage, a first set of leaves being mounted on the first secondary carriage; a second secondary carriage coupled to the primary carriage, a second set of leaves being mounted on the second secondary carriage; and one or more second motors to control movement of leaves the first and second primary carriages.

The particle accelerator may be a synchrocyclotron. The particle therapy system may comprise a gantry on which the synchrocyclotron, the scanning system, and the adaptive aperture are mounted, the gantry being rotatable around a patient to reach the treatment area. The synchrocyclotron may comprise a voltage source to provide a radio frequency (RF) voltage to a cavity to accelerate particles from a particle source, with the voltage source being configured to sweep the RF voltage over a frequency range in a cycle; a coil to receive electrical current having one of multiple values and to generate a magnetic field corresponding to the electrical current, with the magnetic field for causing the particles to move orbitally within the cavity at an energy that corresponds to the electrical current, and with the magnetic field being at least 4 Tesla; and an extraction channel to receive the particles from the cavity and to output the particles received from the cavity to the scanning system, with the particles that are output from the cavity having an energy that corresponds to the electrical current. The synchrocyclotron may be configured to enable setting of the electrical current to one of the multiple values, with each of the multiple values corresponding to a different energy at which particles are output from the cavity. The energy of the particles that are output from the cavity may be variable in a range that is between about 100 MeV and about 300 MeV. The voltage source may be configured to sweep the RF voltage over a different frequency ranges, with each different frequency range corresponding to each different energy at which the particles are output from the cavity.

The synchrocyclotron may comprise a particle source for holding ionized plasma, with the particle source being in a cavity and comprising two parts that are separated at an acceleration region; a voltage source to provide a radio frequency (RF) voltage to the cavity to accelerate particles from the ionized plasma at the separation region of the particle source, with the voltage source being configured to sweep the RF voltage over a frequency range in a cycle; a coil to receive electrical current to generate a magnetic field corresponding to the electrical current, with the magnetic field for causing the particles to move orbitally within the cavity at an energy that corresponds to the electrical current, and with the magnetic field being at least 4 Tesla; at least one magnetic pole piece, with the at least one magnetic pole piece comprising ferromagnetic material that defines a shape of the cavity; and an extraction channel to receive the particles from the cavity and to output the particles received to the scanning system. The energy of the particles that are output from the cavity may be in a range that is between about 100 MeV and about 300 MeV. The voltage source may be configured to sweep the RF voltage over a different frequency ranges, with each different frequency range corresponding to each different energy at which the particles are output from the cavity.

The scanning system may comprise a scanning magnet that is controllable based on a current through the scanning magnet to affect a direction of the particle beam and thereby move the particle beam across the treatment area in the two dimensions; a degrader to change an energy of the particle beam prior to moving the particle beam across the cross-section of the irradiation target, with the degrader being down-beam of the magnet relative to the synchrocyclotron; and a control system (i) to control the current through the scanning magnet in order to produce uninterrupted movement of the beam across at least part of an irradiation target to deliver doses of charged particles, (ii) for positions at which the particle beam delivers dose, to store information identifying a location and an amount of dose delivered, (iii) to compare a cumulative dose delivered at each position to a target cumulative dose, and (iv) if the cumulative dose does not match the target cumulative dose at specific positions, control the current in order to move the beam so as to deliver additional dose to the specific positions. The adaptive aperture may be down-beam of the scanning system relative to the synchrocyclotron.

The adaptive aperture may be configured to mimic a patient-specific aperture. The structures may comprise leaves, at least some of which have shapes that are different from others of the leaves, the at least some of the leaves having curved shapes. The leaves may have edges that are flat. The adaptive aperture may comprise a primary carriage; and secondary carriages on which the leaves are mounted to position the leaves relative to the irradiation target, with the secondary carriages being mounted on the primary carriage, the primary carriage for positioning the secondary carriage. The particle therapy system may comprise curved tracks along which the primary carriage and secondary carriages move.

Also described herein is an adaptive aperture comprising structures that are movable relative to an irradiation target to approximate a shape to trim part of a radiation treatment area of the irradiation target, with the part of the radiation treatment area having a size that is based on an area of the spot size. The example adaptive aperture may include, or be combined with, any appropriate feature(s) set forth in this summary section, either alone or in combination.

The example adaptive aperture may include a relatively small number of motors, cabling, leaves, and other hardware, all of which may have relatively small dimensions. As such, the adaptive aperture may be made smaller than at least some other types of adaptive apertures used in particle therapy. Its small size enables the adaptive aperture to be mounted on the end of a treatment nozzle and, thus, get close to the patient without substantially interfering with treatment. Furthermore, because of its proximity to the patient and its size, the edges of the particle beam that impact the patient may be sharper than those produced by systems that are placed further away from the patient. For example, the adaptive aperture may be located as close as 4 cm from the patient. In an implementation, the adaptive aperture may occupy a space 36 cm×50 cm in area by 10 cm in depth.

Two or more of the features described in this disclosure, including those described in this summary section, may be combined to form implementations not specifically described herein.

Control of the various systems described herein, or portions thereof, may be implemented via a computer program product that includes instructions that are stored on one or more non-transitory machine-readable storage media, and that are executable on one or more processing devices (e.g., microprocessor(s), application-specific integrated circuit(s), programmed logic such as field programmable gate array(s), or the like). The systems described herein, or portions thereof, may be implemented as an apparatus, method, or electronic system that may include one or more processing devices and computer memory to store executable instructions to implement control of the stated functions.

The details of one or more implementations are set forth in the accompanying drawings and the description below. Other features, objects, and advantages will be apparent from the description and drawings, and from the claims.

DESCRIPTION OF THE DRAWINGS

FIG. 1 is a perspective view of an example adaptive aperture leaf that is usable with the example adaptive apertures described herein.

FIG. 2 is a top view of adaptive aperture leaves positioned relative to a treatment area of an irradiation target.

FIG. 3 is a perspective view of an example adaptive aperture.

FIG. 4 is a side view of an example adaptive aperture.

FIG. 5 is a perspective, view of an example adaptive aperture having components portrayed in see-through to show the interiors thereof.

FIG. 6 is a top view of example control structures used to move a leaf into, and out of, a treatment area of an irradiation target.

FIG. 7 is a perspective view of an example adaptive aperture having curved leaves.

FIGS. 8 and 9 are a cross-sectional views of an example synchrocyclotron for use in a particle therapy system.

FIG. 10 is a side view of an example scanning system.

FIG. 11 is a perspective view of components of an example scanning system.

FIG. 12 is a front view of an example magnet for use in a scanning system of the type shown in FIGS. 10 and 11 .

FIG. 13 is a perspective view of an example magnet for use in a scanning system of the type shown in FIGS. 10 and 11 .

FIG. 14 is a perspective view of an example energy degrader (range modulator) for use in a scanning system of the type shown in FIGS. 10 and 11 .

FIG. 15 is a perspective view of a process for moving a leaf of an energy degrader in the path of a particle beam.

FIG. 16 is a perspective view of an adaptive aperture positioned relative to a patient during particle therapy treatment.

FIG. 17 is a flowchart showing an example process for performing raster scanning that may be performed using the hardware of FIGS. 10 to 15 .

FIG. 18 is a top view show an example cross-section of an irradiation target and a radiation scan path.

FIG. 19 is a perspective view of an example therapy system.

FIG. 20 is an exploded perspective view of components of an example synchrocyclotron for use in the particle therapy system.

FIG. 21 is a cross-sectional view of the example synchrocyclotron.

FIG. 22 is a perspective view of the example synchrocyclotron.

FIG. 23 is a cross-sectional view of an example ion source for use in the synchrocyclotron.

FIG. 24 is a perspective view of an example dee leaf and an example dummy dee for use in the synchrocyclotron.

FIG. 25 shows a patient positioned within an example inner gantry of the example particle therapy system in a treatment room.

FIG. 26 is a conceptual view of an example particle therapy system that may use a variable-energy particle accelerator.

FIG. 27 is a perspective, exploded view of an example magnet system that may be used in a variable-energy particle accelerator.

FIG. 28 is an example graph showing energy and current for variations in magnetic field and distance in a particle accelerator.

FIG. 29 is a side view of an example structure for sweeping voltage on a dee leaf over a frequency range for each energy level of a particle beam, and for varying the frequency range when the particle beam energy is varied.

FIG. 30 is a top view of adaptive aperture leaves on carriages mounted on a track that is curved relative to the direction of a particle beam.

FIG. 31 is a top view of adaptive aperture leaves positioned relative to a treatment area of an irradiation target.

Like reference symbols in the various drawings indicate like elements.

DETAILED DESCRIPTION

Described herein are example implementations of an adaptive aperture that may be used to control the extent of radiation, such as a proton or ion beam, applied to a patient. In this regard, an adaptive aperture is a structure that is controllable to allow some radiation to pass to a patient and to block some radiation from passing to the patient. Typically, the radiation that passes is directed to an irradiation target to be treated, and the radiation that is blocked would otherwise hit, and potentially damage, healthy tissue. In operation, the adaptive aperture is placed in the radiation path between a radiation source and an irradiation target and is controlled to produce an opening of an appropriate size and shape to allow some radiation to pass through the opening to the irradiation target, while a remainder of the structure blocks some radiation from reaching adjacent tissue. The adaptive aperture may be used in any appropriate radiation therapy system, and is not limited to use with any particular type of system. Examples of systems with which the adaptive aperture may be used are described herein.

In some implementations, the adaptive aperture contains generally flat structures, which are referred to as “plates” or “leaves”, and which are controllable to move into the “beam” or “treatment” area to block some radiation and allow some radiation to pass. The leaves are controllable to produce an opening of size and shape that is appropriate for the current treatment. In some implementations, the leaves are held on two carriages, and face each other and the treatment area. The leaves are controllable to move into, and out of, the treatment area, to form the opening (or aperture) though which the particle beam passes to treat an area of a patient. The leaves that form the opening also block radiation from passing to tissue (e.g., healthy tissue) adjacent to the opening that is covered by the leaves. In this context, covering includes the leaves blocking the particle beam.

FIG. 1 shows an example of a leaf 40 that may be used in the adaptive aperture, although the adaptive aperture is not limited to use with this type of leaf. The height 50 of the leaf is along the beamline (e.g., the direction of the particle beam). The length 52 of the leaf is along its direction of actuation into and out of the treatment area, and is based on the field size, or portion thereof, that the system can treat. The field size corresponds to the treatment area that the beam can impact. The width 53 of the leaf is the direction along which multiple leaves stack when actuated. Generally, the more leaves that are used, the higher the resolution of the aperture that can be produced, including for curved boundaries.

In FIG. 1 , leaf 40 includes a tongue and groove feature 55 along its side, which is configured to reduce inter-leaf leakage when multiple such leaves stack. In this example, the curved end 56 of leaf 40 is configured to maintain a surface tangent to the beam at all locations in the treatment area. However, as also described herein, the end of each leaf may be flat, not curved.

In some implementations, the adaptive aperture leaves have a height that is sufficient to block at least the maximum beam energy (e.g., the maximum energy of the particle beam output by the system). In some implementations, the adaptive aperture leaves have a height that blocks less than the maximum beam energy, for reasons described below. In some implementations, the adaptive aperture leaves have lengths that are dictated not by the area of an entire treatment area, but rather by the area of a single beam spot or multiple beam spots. In this context, a “beam spot” is the cross-sectional area of a particle beam.

In an example, the particle therapy system may be configured to treat a tumor having a cross-section that can fit into a 20 cm×20 cm square area. In this example, each leaf in the adaptive aperture may have a length of about 2 cm, which is about enough to block particles in half of one beam spot. As noted, the adaptive aperture includes sets of leaves that face each other. So, leaves from each set may be controlled to cover the whole, single beam spot, if necessary, thereby preventing passage of radiation. The leaves may also be controllable to create an opening through which some, or all, of the radiation from the single beam spot can pass.

In operation, the adaptive aperture is configured to move as the beam scans across the radiation target, and to track the beam's movement during scanning. In this example, the adaptive aperture may be configured to move about 20 cm so as to enable coverage over the entirety of the 20 cm×20 cm area. As described above, the adaptive aperture may be configured to use enough leaves to cover (or “trim”) one beam spot and, in some case, a small amount of extra area (e.g., 5% extra area, 10% extra area, 15% extra area, or 20% extra area).

FIG. 2 shows an example implementation of an adaptive aperture 700. Adaptive aperture 700 includes leaves 701 having a height and made of a material, such as nickel, brass, tungsten, or other metal, sufficient to inhibit or prevent passage of radiation at a given energy. For example in some systems, a particle accelerator is configured to generate a particle beam having a maximum energy of 100 MeV to 300 MeV. Accordingly, in such systems, the leaves may be constructed to prevent passage of a beam having an energy of 100 MeV, 150 MeV, 200 MeV, 250 MeV, 300 MeV, and so forth.

Leaves

701 are mounted on carriages to control their movement relative to a treatment area of an irradiation target, such as a cross-sectional layer of a tumor in a patient. The movement is controlled to cause leaves 701 to cover some parts of treatment area 704, thereby preventing radiation from impacting those parts during treatment, while leaving other parts of treatment area exposed to the radiation. In the example implementation of FIG. 2 , there are fourteen leaves in total, seven on the left and seven on the right. In some implementations, there may be a different number of leaves, e.g., ten in total, five on the left and five on the right, twelve in total, six on the left and six on the right, and so forth.

The adaptive aperture may be used with any appropriate type of radiation therapy system. In an example implementation, the radiation therapy system is a proton therapy system. As described herein, an example proton therapy system scans a proton beam across a treatment area of an irradiation target in order to destroy malignant tissue. During scanning, the particle beam moves across the treatment area to cover the treatment area with radiation. In an example implementation, the particle beam is pulsed. Because the particle beam is pulsed, the affected parts of the treatment area constitute a series of spots, one for each pulse that hits the treatment area. Depending upon the size of the beam, the result may leave some areas untreated. As a result, it may be beneficial to scan the same treatment area more than once in order to ensure that the entire area is treated. Each successive scan may be offset from the other(s) in order to hit all areas. An example of this type of scanning is called pencil-beam scanning, and the repetitive scans are referred to as painting or repainting the treatment area.

The irradiation target is typically three-dimensional in structure. Accordingly, as described herein, the irradiation target is treated cross-sectional layer (or simply “layer”) by layer. That is, a layer of the irradiation target is treated, followed by another treatment of another layer, and so forth until the entire target is treated. Different layers of an irradiation target are treated by varying an energy level of the particle beam. That is, different energy levels of the particle beam impact different layers of the irradiation target, with higher energy levels affecting layers deeper inside the irradiation target relative to the particle beam source. Accordingly, during treatment, the energy level of the particle beam is changed in order to reach, and thus treat, different layers of the irradiation target.

FIG. 2 shows leaves 701 configured allow radiation to impact part of a layer (e.g., the treatment area) and to prevent radiation from impacting other parts of the layer (e.g., healthy tissue). In FIG. 1 , locations 707 represent centers of beam spots to be delivered during a scan of a proton beam across treatment area 704. Circle 708 represents a treatment boundary beyond which no radiation is intended to be delivered. Beam spots that are close to this boundary (e.g., within one standard deviation of the particle beam's profile) border healthy tissue. These are spots that are trimmed (that is, blocked) by appropriate configuration and placement of leaves on the adaptive aperture. An example of a beam spot to be trimmed is beam spot 711, having its center at location 706. As shown, leaves 701 are configured to block the portion of beam spot 711 that extends beyond circle 708.

In an example implementation, on each of two separate carriages, there are five leaves that are about 5 mm in width and two leaves that are about 20 mm in width. In some implementations, on each of two separate carriages, there are seven leaves, two of which each have widths that are three times or more the widths of each of five other leaves. Other implementations may contain different numbers, sizes, and configurations of leaves, and different numbers and configurations of carriages. For example, some implementations may include any number between five and fifty leaves per carriage, e.g., 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26, 27, 28, 29, 30, 31, 32, 33, 34, 35, 36, 37, 38, 39, 40, 41, 42, 43, 44, 45, 46, 47, 48, 49, or 50 leaves (or more) per carriage.

The carriages can move both horizontally and vertically, as described herein. The leaves are also movable horizontally relative to each carriage into, and out of, the treatment area. In this way, the leaves are configurable to approximate the shape of the treatment boundary in the region near the area being treated (e.g., circle 711 or a portion thereof in this example).

The leaves may be moved vertically and/or horizontally between different scans of the particle beam so that the leaves are in appropriate positions when the beam is delivered to a particular area. The leaves need not necessarily be moved for every scan pass, but instead may be moved to a location appropriate for an area. In some cases, e.g., for spots interior to the treatment area, radiation treatment may proceed without the trimming provided by the adaptive aperture.

FIG. 31 shows another example of leaves 1400 that are part of an adaptive aperture configured to trim a radiation spot 1401 centered at location 1402. In this example, there are seven leaves on each of two sides of the adaptive aperture (supported by corresponding carriages). The leaves on each side include two leaves that are wider than the other five; however, the adaptive aperture is not limited to this configuration. In this case, spot 1401 has a radius of 2.5 sigma defining an 8 mm Gaussian radiation spot.

FIGS. 3, 4, and 5 show an example implementation of

carriages

713, 714, 715 configured to hold, and to move, the leaves described above both vertically and horizontally relative to the treatment target. As shown, vertical movement includes movement in the Cartesian Z-direction 717, and horizontal movement includes movement in the Cartesian X direction 718 (with the Cartesian Y direction being into, or out of, the page in FIG. 4 ). FIGS. 4 and 5 show parts of carriage housings as transparent in order to show components inside the housings; however, the housings are not actually transparent.

Carriage

713 is referred to herein as the primary carriage, and

carriages

714 and 715 are referred to herein as secondary carriages.

Secondary carriages

714, 715 are coupled to primary carriage 713, as shown in FIGS. 3 to 5 . In this example,

secondary carriages

714, 715 each include a housing that is fixed to primary carriage 715 via a corresponding

member

718, 719. In this example, primary carriage 713 is movable vertically relative to the irradiation target and relative to particle accelerator along tracks 720. The vertical movement of primary carriage 713 also causes the secondary carriages to move vertically. In some implementations, the secondary carriages move vertically in concert. In some implementations, vertical movement of each secondary carriage is independent of vertical movement of the other secondary carriage.

As shown in FIGS. 3 to 5 , each

secondary carriage

714, 715 is connected to a

corresponding rod

722, 723, along which the secondary carriage moves. More specifically, in this example, motor 725 drives secondary carriage 714 to move along rod 722 towards or away from secondary carriage 715. Likewise, in this example, motor 726 drives secondary carriage 715 to move along rod 723 towards or away from secondary carriage 714. Control over movement of the primary and secondary carriages is implemented to position the leaves relative to the irradiation target, as described herein. In addition, the leaves themselves are also configured to move in and out of the carriages, as also described herein.

As shown in FIG. 5 , a motor 730 drives the vertical movement of primary carriage 713. For example, as shown in FIG. 3 , lead screw 731 is coupled to housing 732, which holds

motors

725, 726 that drive corresponding

secondary carriages

714, 715, and which is mounted on tracks 720. Lead screw 731 is coupled to, and driven vertically by, motor 730. That is, motor 730 drives lead screw 731 vertically, either towards or away from the irradiation target. Because lead screw 731 is fixed to housing 732, this movement also causes housing 732, and thus

secondary carriages

714, 715, to move along tracks 720, either towards or away from the irradiation target.

In this example implementation, as noted, seven leaves 735, 736 are mounted on each

secondary carriage

714, 715. Each secondary carriage may be configured to move its leaves horizontally into, or out of, the treatment area. The individual leaves on each secondary carriage may be independently movable in the X direction relative to other leaves on the same secondary carriage. In some implementations, the leaves may also be configured to move in the Y direction. Furthermore, the leaves on one secondary carriage 714 may be movable independently of the leaves on the other secondary carriage 715. These independent movements of leaves on the secondary carriages, together with the vertical movements enabled by the primary carriage, allow the leaves to be moved into various configurations. As a result, the leaves can conform, both horizontally and vertically, to treatment areas that are randomly shaped both in horizontal and vertical dimensions. The sizes and shapes of the leaves may be varied to create different conformations.

The leaves may be made of any appropriate material that prevents or inhibits transmission of radiation. The type of radiation used may dictate what material(s) are used in the leaves. For example, if the radiation is X-ray, the leaves may be made of lead. In the examples described herein, the radiation is a proton or ion beam. Accordingly, different types of metals or other materials may be used for the leaves. For example, the leaves may be made of nickel, tungsten, lead, brass, steel, iron, or any appropriate combinations thereof. The height of each leaf may determine how well that leaf inhibits transmission of radiation.

In some implementations, the leaves may have the same height, whereas in other implementations, some of the leaves may have heights that are different from heights of others of the leaves. For example, in FIGS. 2 to 5 , the leaves are each 5 mm in height. However, any appropriate heights may be used. For example, leaves 735, 736 may have any of the following (or other heights): 1 mm, 2 mm, 3 mm, 4 mm, 5 mm, 6 mm, 7 mm, 8 mm, 9 mm, 10 mm, 11 mm, 12 mm, 13 mm, 14 mm, 15 mm, 16 mm, 17 mm, 18 mm, 19 mm, 20 mm, 21 mm, 22 mm, 23 mm, 24 mm, 25 mm, 26 mm, 27 mm, 28 mm, 29 mm, and so forth. The leaves may have any combination of the foregoing heights. In addition, each of the leaves may have a different height than one or more others of the leaves.

Leaves of the same height or of varying heights may be stacked to inhibit radiation transmission. In some implementations, shorter leaves (e.g., leaves of lesser height) may be used in connection with longer leaves. In some implementations, the leaves have enough height to completely block the particle beam at the maximum beam energy. In some implementations, the leaves have enough height to block the particle beam at less than the maximum beam energy (and not to block the particle beam at maximum energy). For example, while a proton therapy system may have the capability to deliver a beam of energy 230 MeV that can treat to a depth in the patient of 32 cm, in some implementations, the adaptive aperture can only block protons of at most 175 MeV that can treat to a depth of no more than 20 cm. In doing so, less beam-stopping material may be used, e.g., 2.1 cm of Tungsten instead of 3.3 cm, or 3.3 cm of Nickel instead of 5.2 cm. In this example, the proton therapy system would still be capable of treating at depths exceeding 20 cm, but the adaptive aperture would not be used for such treatments. This may be deemed acceptable because, in some circumstances, deeper treatments benefit less from the particle beam collimation that the adaptive aperture provides. That is, in some treatment scenarios, shallow, low-energy treatments are where the adaptive aperture will be most effective, and there may be engineering advantages to reducing the amount of material in the leaves. Thus, in some example implementations, shorter leaves are used and the adaptive aperture is restricted to use with shallow, lower-than-maximum energy treatments.

In the implementations of FIGS. 2 to 5 , the leaves are semi-rectangular in shape and have about the same surface area when viewed from the side. In some implementations, this need not be the case. For example, the leaves may have different shapes than those shown. Example shapes include, but are not limited to, circular shapes, curvilinear shapes, oval shapes, square shapes, and triangular shapes. Furthermore, individual leaves may have different shapes than others of the leaves contained in the same carriage or in a different carriage. For example, one carriage may contain both rectangular and curvilinear shaped leaves.

In some implementations, the leaves have heights that are enough not only to fully stop a particle beam at the maximum expected proton energy (e.g., 3.3 cm of Tungsten at 230 MeV or, e.g., 5.2 cm of nickel), but also to have enough extra material to prevent proton transmission between the leaves. This material may have a tongue and groove structure as shown in FIG. 1 , or a similar configuration. The leaf ends may be configured to include curved or tapered surfaces to enhance delivered penumbra for proton beams of various divergence.

In some implementations, there may be more than one primary carriage and corresponding motors and rails. For example, a first primary carriage may control vertical movement of a first secondary carriage, and a second primary carriage may control vertical movement of a second secondary carriage. Therefore, in such implementations, the two secondary carriages can be moved independently in the vertical dimension, if desired. In any case, the primary carriage may be computer controlled. For example, executable instructions are stored in computer memory (e.g., one or more non-transitory machine-readable storage media), and executed by one or more processing devices to control the movement. Control may be performed with, or without, user input during treatment.

As explained, each

secondary carriage

714, 715 includes a corresponding motor to control horizontal carriage movement, as described above. In some implementations, there may be one motor for each leaf, whereas in other implementations a single motor may control all leaves. The motors may be mounted on a corresponding secondary carriage. As a result, the motors move vertically along with the corresponding secondary carriage. As noted, the motors control movement of leaves in each carriage. The leaves are mounted on actuators that enable movement in two dimensions. In the examples of FIGS. 2 to 5 , the leaves are each part of an integrated leaf. Referring to the example of FIG. 6 , mechanisms enable the individual leaves to move in and out (the X direction) of the integrated leaf that comprises each carriage into, or out of, the treatment area.

In some implementations, all leaves on a single carriage are independently movable. FIG. 6 shows the movement mechanism for a leaf 735 a that is part of a secondary carriage. Each leaf in each secondary carriage may have a configuration, and movement mechanism, that is similar to, or identical to, the leaf and movement mechanism of FIG. 6 .

In the example of FIG. 6 , the movement mechanism includes a leaf stick 735 b, a lead screw nut 735 c, a lead screw 735 d, a thrust bearing assembly 735 e, a coupling 735 f, a motor 735 g, a bearing block 735 h, a sleeve bearing pin 735 i, a sleeve bearing 735 j, and a motor mount block 735 k. In operation the motor shaft, through the coupling, spins the lead screw. This causes the lead screw nut to advance or retract depending on the direction of screw rotation. The lead screw nut is fixed to the leaf assembly so the leaf is moved forward or backward (into or out of the beam path) as the motor spins. Sleeve bearing pins are fixed to the leaf and slide along sleeve bearings which are held captive in the bearing block that supports the whole assembly. This bearing block houses the bearings and provides space for the motor assemblies for all leaves on the carriage.

As described, the adaptive aperture can be used to trim each layer of a scanned treatment with a different aperture shape, allowing for three-dimensional field shaping techniques such as layer stacking. However, an implementation of the adaptive aperture may be configured to mimic either a machined patient-specific structure or a multi-leaf collimator.

In this regard, existing treatment planning systems (TPSs) typically include the capability to calculate the shape of a fixed brass aperture meant to be uniformly applied to the entire treatment volume. TPSs may also dictate, or contain instructions to configure, an adaptive aperture shape for a target. A computer program can interpret an aperture shape, either from a continuous aperture curve or set of fixed multi-leaf collimator leaf positions, and translate that shape into a series of dynamic leaf positions for the adaptive aperture that correlate with delivered radiation treatment spots. Existing TPS functionality can thus be leveraged, allowing the adaptive aperture to be compatible, with relatively few modifications, to existing TPS software.

Another example technique that may improve edge conformality and that is enabled by the adaptive aperture takes advantage of the possibility that a treatment dose to the same treatment area of a layer will be delivered in several passes or paintings. Repainting, which is described herein, is a technique used in scanned proton therapy in which dose is divided to a treatment area using several particle beam passes in order to spread the delivered radiation uniformly during a timescale that is long compared with patient motion, such as breathing. There are also other reasons in which dose to a given spot may not all be delivered in one pulse. Some example reasons include: dynamic dose control can regulate the charge in each pulse to deliver an accurate total dose, there are safety limits to the charge in a pulse, and a required dynamic range of dose may exceed the capabilities of the particle accelerator.

If the spots in an irradiated volume will be painted several times during a treatment (e.g., during multiple scans), then the conformality of the adaptive aperture to the lateral edge of the irradiation target can be improved by shifting the leaves slightly (e.g., at the sub-millimeter level), vertically, horizontally, or both vertically and horizontally between each painting (e.g., between each scan pass of the particle beam covering a same treatment area). In this way, what might have been a slightly jagged edge owing to the finite size of the individual leaves can be smoothed to attain a better approximation of the intended aperture curve.

Adding rotational degrees of freedom can improve the ability of the adaptive aperture to conform to radiation targets. For example, the entirety of the assembly of FIGS. 3 to 5 may be configured to be rotated in a plane perpendicular to the beam direction, in a plane parallel to the beam direction, or in a combination thereof. In some implementations, each individual

secondary carriage

714, 715 may be configured to rotate independently in a same plane. In this way, the adaptive aperture may provide more flexibility to conform to complex shapes that are not ideally oriented. In some implementations, both the primary carriage and each secondary carriage may be rotatable.

In the example implementations described above, each leaf is independently actuated such that an arbitrary shape can be traced with a leaf configuration. It may be, however, that such flexibility is not required to achieve acceptable edge conformality. The leaves could be mechanically constrained with the ability to achieve only a finite number of configurations. For example, the leaves could be restricted to arrangements that put them in a vertical line, forward diagonal shape, backward diagonal shape, concave shape, convex shape, or any other achievable shape. In this way, flexibility could be traded for mechanical simplicity. The leaves may be actuated using a cam timing leaf through one remote motor rather than four motors mounted on a secondary carriage. In some implementations, discrete shapes of the leaves may be machined out of sectors of wheels which are rotated into place as needed. In order to reduce the number of motors, feedback, controllers, and associated wiring, an assembly may be used that has one motor that achieves discrete leaf configurations.

FIG. 7 shows an example implementation of an adaptive aperture having curved leaves 750 that are rotatable relative to shaft 751. In the example of FIG. 7 , all leaves are actuated by one motor. This motor is at the top of vertical shaft 751. The shape and orientations of leaf cams are chosen to achieve different leaf configurations for different rotational angles of the main drive shaft.

Another possible advantage of the adaptive aperture is the ability to collimate edges that are completely internal to the field. If a treatment plan calls for a volume to be treated that completely surrounds a volume to be protected—for example, a tumor that completely surrounds a spinal cord—a single, machined structure will typically be unable to block radiation to the protected volume without blocking some of treated volume as well. The adaptive aperture can treat such a field using a sequence of leaf positions. For example, the adaptive aperture can be reconfigured dynamically, and during treatment, to protect the areas that require protection, while allowing treatment on areas that require treatment.

In some cases, better beam performance (penumbra or edge sharpness) results when the particle beam is tangent to the surface of a leaf edge. However, since the beam effectively originates from a single point source, the angle with which it passes through the plane of the adaptive aperture changes as the beam is moved away from the center of the field. For this reason, leaves often have curved edges, as shown in FIG. 1 , so that the edges can always be placed a location that makes them tangent to the particle beam. In an example implementation of the adaptive aperture, the tracks on which both primary and secondary carriages move are curved so that flat leaf edges can be used in lieu of curved leaf edges, and so that the flat but remain tangent to the particle beam.

FIG. 30 shows an example implementation of a curved track 1420. In the example of FIG. 30 , the particle beam 1421 originates from source 1422, which may be a particle accelerator like the synchrocyclotron described herein. Particle beam 1422 may scan through field 1423 and, at one extent, may be at location 1425 and, at another extent, may be at location 1426.

Carriages holding leaves

1428 and 1429 are mounted on curved track 1420 so that leaves 1428 and 1428 can move towards or away from each other. In this example, the leaves have straight ends (or “fronts”) 1431, 1431 in contrast to curved end 56 of FIG. 1 . By employing a curved track, the particle beam can remain tangent, or substantially tangent, to the straight ends throughout the scan field 1423. Keeping the particle beam tangent to the ends can be advantageous in that it enables the trimming provided by the adaptive aperture to be consistent throughout the range of the beam field.

To summarize, in some implementations, the adaptive aperture trims only a small fraction of a treatment area at one time, e.g., an area that is less than the entire treatment area and that is about equal to one spot size, two spot sizes, three spots sizes, four spot sizes, five spot sizes, and so forth. Thus, in some implementations, the adaptive aperture may be small enough to trim a single spot at once and may be large enough to trim several spots in one position, but not the entire field without moving. Thus, the adaptive aperture may be configured to move around and within the field as the beam scans. That is, in some implementations, the adaptive aperture tracks the beam as it scans, and its configuration and reconfiguration may be synchronized to the scanning and to the pulses provided by the beam (e.g., different reconfigurations for different beam pulses and/or locations). By not using leaves large enough to trim an entire treatment area, the adaptive aperture can be made smaller and therefore the adaptive aperture can be placed closer to the patient with little or no interference from other devices. In some implementations, no leaf of the adaptive aperture even has one dimension that spans an entire maximum treatment area. In some implementations, each individual leaf is movable in two dimensions within the treatment area, and the device is mounted on a gantry (e.g., in the context of a particle therapy system such as that described herein) to be rotated on one or more axes and made extendable towards and away from isocenter.

Also described herein is an example of a particle accelerator system, such as a proton or ion therapy system, which may employ an adaptive apertures of FIGS. 1 to 7, 30, and 31 . The example particle therapy system includes a particle accelerator—in this example, a synchrocyclotron—mounted on a gantry. The gantry enables the accelerator to be rotated around a patient position, as explained in more detail below, to allow a particle beam from the particle accelerator hit any arbitrary treatment area in the patient. In some implementations, the gantry is steel and has two legs mounted for rotation on two respective bearings that lie on opposite sides of a patient. The particle accelerator is supported by a steel truss that is long enough to span a treatment area in which the patient lies and that is attached at both ends to the rotating legs of the gantry. As a result of rotation of the gantry around the patient, the particle accelerator also rotates.

In an example implementation, the particle accelerator (e.g., the synchrocyclotron) includes a cryostat that holds one or more superconducting coils, each for conducting a current that generates a magnetic field (B). In an example, the cryostat uses liquid helium (He) to maintain each coil at superconducting temperatures, e.g., 4° Kelvin (K). Magnetic yokes or smaller magnetic pole pieces are located inside the cryostat, and define the shape of a cavity in which particles are accelerated. Magnetic shims may pass through the magnetic yokes or pole pieces to change the shape and/or magnitude of the magnetic field in the cavity.

In this example implementation, the particle accelerator includes a particle source (e.g., a Penning Ion Gauge—PIG source) to provide an ionized plasma column to the cavity. Hydrogen gas is ionized to produce the plasma column. A voltage source provides a radio frequency (RF) voltage to the cavity to accelerate pulses of particles from the plasma column into the cavity. The magnetic field in the cavity is shaped to cause particles to move orbitally within the cavity. The magnetic field may be, e.g., at least 4 Tesla, as explained herein.

As noted, in an example, the particle accelerator is a synchrocyclotron. Accordingly, the RF voltage is swept across a range of frequencies to account for relativistic effects on the particles (e.g., increasing particle mass) when accelerating particles from the plasma column. The magnetic field produced by running current through a superconducting coil, together with the shape of the cavity, causes particles accelerated from the plasma column to accelerate orbitally within the cavity. In other implementations, a particle accelerator other than a synchrocyclotron may be used. For example, a cyclotron, a synchrotron, a linear accelerator, and so forth may be substituted for the synchrocyclotron described herein.

In the example synchrocyclotron, a magnetic field regenerator (“regenerator”) is positioned near the outside of the cavity (e.g., at an interior edge thereof) to adjust the existing magnetic field inside the cavity to thereby change locations (e.g., the pitch and angle) of successive orbits of the particles accelerated from the plasma column so that, eventually, the particles output to an extraction channel that passes through the cryostat. The regenerator may increase the magnetic field at a point in the cavity (e.g., it may produce a magnetic field “bump” of about 2 Tesla or so at an area of the cavity), thereby causing each successive orbit of particles at that point to precess outwardly toward the entry point of the extraction channel until it reaches the extraction channel. The extraction channel receives, from the cavity, particles accelerated from the plasma column and outputs the received particles from the cavity as a particle beam.

The superconducting (“main”) coils can produce relatively high magnetic fields. The magnetic field generated by a main coil may be within a range of 4 T to 20 T or more. For example, a main coil may be used to generate magnetic fields at, or that exceed, one or more of the following magnitudes: 4.0 T, 4.1 T, 4.2 T, 4.3 T, 4.4 T, 4.5 T, 4.6 T, 4.7 T, 4.8 T, 4.9 T, 5.0 T, 5.1 T, 5.2 T, 5.3 T, 5.4 T, 5.5 T, 5.6 T, 5.7 T, 5.8 T, 5.9 T, 6.0 T, 6.1 T, 6.2 T, 6.3 T, 6.4 T, 6.5 T, 6.6 T, 6.7 T, 6.8 T, 6.9 T, 7.0 T, 7.1 T, 7.2 T, 7.3 T, 7.4 T, 7.5 T, 7.6 T, 7.7 T, 7.8 T, 7.9 T, 8.0 T, 8.1 T, 8.2 T, 8.3 T, 8.4 T, 8.5 T, 8.6 T, 8.7 T, 8.8 T, 8.9 T, 9.0 T, 9.1 T, 9.2 T, 9.3 T, 9.4 T, 9.5 T, 9.6 T, 9.7 T, 9.8 T, 9.9 T, 10.0 T, 10.1 T, 10.2 T, 10.3 T, 10.4 T, 10.5 T, 10.6 T, 10.7 T, 10.8 T, 10.9 T, 11.0 T, 11.1 T, 11.2 T, 11.3 T, 11.4 T, 11.5 T, 11.6 T, 11.7 T, 11.8 T, 11.9 T, 12.0 T, 12.1 T, 12.2 T, 12.3 T, 12.4 T, 12.5 T, 12.6 T, 12.7 T, 12.8 T, 12.9 T, 13.0 T, 13.1 T, 13.2 T, 13.3 T, 13.4 T, 13.5 T, 13.6 T, 13.7 T, 13.8 T, 13.9 T, 14.0 T, 14.1 T, 14.2 T, 14.3 T, 14.4 T, 14.5 T, 14.6 T, 14.7 T, 14.8 T, 14.9 T, 15.0 T, 15.1 T, 15.2 T, 15.3 T, 15.4 T, 15.5 T, 15.6 T, 15.7 T, 15.8 T, 15.9 T, 16.0 T, 16.1 T, 16.2 T, 16.3 T, 16.4 T, 16.5 T, 16.6 T, 16.7 T, 16.8 T, 16.9 T, 17.0 T, 17.1 T, 17.2 T, 17.3 T, 17.4 T, 17.5 T, 17.6 T, 17.7 T, 17.8 T, 17.9 T, 18.0 T, 18.1 T, 18.2 T, 18.3 T, 18.4 T, 18.5 T, 18.6 T, 18.7 T, 18.8 T, 18.9 T, 19.0 T, 19.1 T, 19.2 T, 19.3 T, 19.4 T, 19.5 T, 19.6 T, 19.7 T, 19.8 T, 19.9 T, 20.0 T, 20.1 T, 20.2 T, 20.3 T, 20.4 T, 20.5 T, 20.6 T, 20.7 T, 20.8 T, 20.9 T, or more. Furthermore, a main coil may be used to generate magnetic fields that are within the range of 4 T to 20 T (or more, or less) that are not specifically listed above.

In some implementations, such as the implementation shown in FIGS. 8 and 9 , large ferromagnetic magnetic yokes act as a return for stray magnetic field produced by the superconducting coils. For example, in some implementations, the superconducting magnet can generate a relatively high magnetic field of, e.g., 4 T or more, resulting in considerable stray magnetic fields. In some systems, such as that shown in FIGS. 8 and 9 , the relatively large ferromagnetic return yoke 100 is used as a return for the magnetic field generated by superconducting coils. A magnetic shield surrounds the yoke. The return yoke and the shield together dissipated stray magnetic field, thereby reducing the possibility that stray magnetic fields will adversely affect the operation of the accelerator.

In some implementations, the return yoke and shield may be replaced by, or augmented by, an active return system. An example active return system includes one or more active return coils that conduct current in a direction opposite to current through the main superconducting coils. In some example implementations, there is an active return coil for each superconducting coil, e.g., two active return coils—one for each superconducting coil (referred to as a “main” coil). Each active return coil may also be a superconducting coil that surrounds the outside of a corresponding main superconducting coil concentrically.

Current passes through the active return coils in a direction that is opposite to the direction of current passing through the main coils. The current passing through the active return coils thus generates a magnetic field that is opposite in polarity to the magnetic field generated by the main coils. As a result, the magnetic field generated by an active return coil is able to dissipate at least some of the relatively strong stray magnetic field resulting from the corresponding main coil. In some implementations, each active return may be used to generate a magnetic field of between 2.5 T and 12 T or more. For example, the magnetic field may be 2.5 T, 2.6 T, 2.7 T, 2.8 T, 2.9 T, 3.0 T, 3.1 T, 3.2 T, 3.3 T, 3.4 T, 3.5 T, 3.6 T, 3.7 T, 3.8 T, 3.9 T, 4.0 T, 4.1 T, 4.2 T, 4.3 T, 4.4 T, 4.5 T, 4.6 T, 4.7 T, 4.8 T, 4.9 T, 5.0 T, 5.1 T, 5.2 T, 5.3 T, 5.4 T, 5.5 T, 5.6 T, 5.7 T, 5.8 T, 5.9 T, 6.0 T, 6.1 T, 6.2 T, 6.3 T, 6.4 T, 6.5 T, 6.6 T, 6.7 T, 6.8 T, 6.9 T, 7.0 T, 7.1 T, 7.2 T, 7.3 T, 7.4 T, 7.5 T, 7.6 T, 7.7 T, 7.8 T, 7.9 T, 8.0 T, 8.1 T, 8.2 T, 8.3 T, 8.4 T, 8.5 T, 8.6 T, 8.7 T, 8.8 T, 8.9 T, 9.0 T, 9.1 T, 9.2 T, 9.3 T, 9.4 T, 9.5 T, 9.6 T, 9.7 T, 9.8 T, 9.9 T, 10.0 T, 10.1 T, 10.2 T, 10.3 T, 10.4 T, 10.5 T, 10.6 T, 10.7 T, 10.8 T, 10.9 T, 11.0 T, 11.1 T, 11.2 T, 11.3 T, 11.4 T, 11.5 T, 11.6 T, 11.7 T, 11.8 T, 11.9 T, 12.0 T, or more. Furthermore, an active return coil may be used to generate magnetic fields that are within the range of 2.5 T to 12 T (or more, or less) that are not specifically listed above.

Referring to FIG. 10 , at the output of extraction channel 102 of particle accelerator 105 (which may have the configuration shown in FIGS. 8 and 9 ), is an example scanning system 106 that may be used to scan the particle beam across at least part of an irradiation target. FIG. 11 also shows examples of components of the scanning system. These include, but are not limited to, a scanning magnet 108, an ion chamber 109, and an energy degrader 110. Other components that may be incorporated into the scanning system are not shown in FIG. 11 , including, e.g., one or more scatterers for changing beam spot size. The example scanning system, including components thereof, may be mounted to the gantry and move along with the particle accelerator during movement of the gantry.

In an example operation, scanning magnet 108 is controllable in two dimensions (e.g., Cartesian XY dimensions) to direct the particle beam across a treatment area (e.g., a cross-section) of an irradiation target. Ion chamber 109 detects the dosage of the beam and feeds-back that information to a control system to adjust beam movement. Energy degrader 110 is controllable to move material (e.g., one or more individual plates) into, and out of, the path of the particle beam to change the energy of the particle beam and therefore the depth to which the particle beam will penetrate the irradiation target. In this way, the energy degrader selects a depth-wise layer of an irradiation target to scan in two dimensions.

FIGS. 12 and 13 show views of an example scanning magnet 108. In this example implementation, scanning magnet 108 includes two coils 111, which control particle beam movement in the X direction, and two coils 112, which control particle beam movement in the Y direction. Control is achieved, in some implementations, by varying current through one or both sets of coils to thereby vary the magnetic field(s) produced thereby. By varying the magnetic field(s) appropriately, the particle beam can be moved in the X and/or Y direction across the irradiation target. In some implementations, the scanning magnet is not movable physically relative to the particle accelerator. In other implementations, the scanning magnet may be movable relative to the particle accelerator (e.g., in addition to the movement provided by the gantry). In some implementations, the scanning magnet may be controllable to move the particle beam continuously so that there is uninterrupted motion of the particle beam over at least part of, and possibly all of, a layer of an irradiation target being scanned or a portion thereof (e.g., a treatment area). In other implementations, the scanning magnets are controllable at intervals or specific times. In some implementations, there may be different scanning magnets to control all or part movement of a particle beam in the X and/or Y directions.

In some implementations, scanning magnet 108 may have an air core. In other implementations, scanning magnet 108 may have a ferromagnetic (e.g., an iron) core. In general, a magnet having an air core includes a magnetic coil around a core that is a non-ferromagnetic material, such as air. For example, an air core magnet may include self-supporting coils that surround air. In some implementations, an air core magnet may include coils that are wound around an insulator, such as ceramic or plastic, which may or may not include air.

In some cases, an air core may have advantages over a ferromagnetic core. For example, the amount that the particle beam moves (e.g., is deflected) in the X and/or Y directions is determined, at least in part, based on the amount of current applied to the magnet (referred to as the “magnet current”). A scanning magnet typically has a movement (or deflection) range, which is the extent over which the magnet will move the beam. At extremes of this range, such as at the edges, larger amounts of current are applied to the scanning magnet in order to achieve relatively high amounts of beam deflection. Some types of scanning magnets having a ferromagnetic core may saturate at these extremes, resulting in a non-linear relationship between current and magnet movement. That is, the amount of deflection produced by the magnet may not be linearly proportional to the amount of current applied to the magnet. Due to this non-linearity, in some cases, it may be difficult to determine and/or set some beam locations using magnet current. Accordingly, when a scanning magnet having a ferromagnetic core is used, there may need to be some calibration and/or compensation performed in order to correct for non-linearities such as that described above.

In contrast, a scanning magnet having an air core may not saturate in the same manner as a scanning magnet having a ferromagnetic core. For example, an air core magnet may not saturate or may saturate less than a magnet having a ferromagnetic core. As a result, the relationship between current and magnet movement may be more linear, particularly at the range extremes, making determinations of beam location based on magnet current more accurate, at least in some cases. This increased linearity also can enable more accurate movement of the beam, particularly at range extremes. That is, since the relationship between current and beam movement is generally more linear over a larger range when an air core scanning magnet is used, beam movement may be more easily reproducible using an air core scanning magnet. This can be advantageous, since a depth-wise layer of an irradiation target may require multiple scans, each providing a percentage of a total cumulative radiation dose. Precision in delivery of multiple doses to the same area, such as that which can be obtained through use of an air core scanning magnet, can affect the efficacy of the treatment.

Although the relationship between current and magnet movement may be more linear in an air core magnet, in some cases, an air core magnet may be more susceptible to stray magnetic fields than a magnet having a ferromagnetic core. These stray magnetic fields may impact the scanning magnet during motion of the scanning magnet produced by the gantry. Accordingly, in some implementations that use a scanning magnet having an air core, the current applied to the scanning magnet to move the beam may be calibrated to account for the position of the scanning magnet relative to the patient (or, correspondingly, to account for the position of the gantry, since the position of the gantry corresponds to the position of the scanning magnet relative to the patient). For example, the behavior of the scanning magnet may be determined and, if necessary, corrected, for different rotational positions (angles) of the gantry, e.g., by increasing or decreasing some applied current based on rotational position.

In some implementations, the scanning magnet may have a core that is comprised of both air and a ferromagnetic material (e.g., iron). In such implementations, the amount and configuration of air and ferromagnetic material in the core may be determined taking the foregoing factors into account.

In some implementations, a current sensor 118 may be connected to, or be otherwise associated with, scanning magnet 108. For example, the current sensor may be in communication with, but not connected to, the scanning magnet. In some implementations, the current sensor samples current applied to the magnet, which may include current to coil(s) for controlling beam scanning in the X direction and/or current to coil(s) for controlling beam scanning in the Y direction. The current sensor may sample current through the magnet at times that correspond to the occurrence of pulses in the particle beam or at a rate that exceeds the rate that the pulses occur in the particle beam. In the latter case, the samples, which identify the magnet current, are correlated to detection of the pulses by the ion chamber described below. For example, the times at which pulses are detected using the ion chamber (described below) may be correlated in time to samples from the current sensor, thereby identifying the current in the magnet coil(s) at the times of the pulses. Using the magnet current, it thus may be possible to determine the location on the irradiation target (e.g., on a depth-wise layer of the irradiation target) where each pulse, and thus dose of particles, was delivered. The location of the depth-wise layer may be determined based on the position of the energy degrader (e.g., the number of plates) in the beam path.

During operation, the magnitude(s) (e.g., value(s)) of the magnet current(s) may be stored for each location at which a dose is delivered, along with the amount (e.g., intensity) of the dose. A computer system, which may be either on the accelerator or remote from the accelerator and which may include memory and one or more processing devices, may correlate the magnet current to coordinates within the irradiation target, and those coordinates may be stored along with the amount of the dose. For example, the location may be identified by depth-wise layer number and Cartesian XY coordinates or by Cartesian XYZ coordinates (with the layer corresponding to the Z coordinate). In some implementations, both the magnitude of the magnet current and the coordinate locations may be stored along with the dose at each location. This information may be stored in memory either on, or remote from, the accelerator. As described in more detail herein, this information may be used during scanning to apply multiple doses to the same locations to achieve target cumulative doses.

In some implementations, ion chamber 109 detects dosage (e.g., one or more individual doses) applied by the particle beam to positions on an irradiation target by detecting the numbers of ion pairs created within a gas caused by incident radiation. The numbers of ion pairs correspond to the dose provided by the particle beam. That information is fed-back to the computer system and stored in memory along with the time that the dose is provided. This information may be correlated to, and stored in association with, the location at which the dose was provided and/or the magnitude of the magnet current at that time, as described above.

As described in more detail below, in some implementations, the scanning system is run open loop, in which case the particle beam is moved freely and uninterrupted across an irradiation target so as to substantially cover the target with radiation. As the radiation is delivered, dosimetry implemented by the particle therapy control system records (e.g., stores) the amount of the radiation per location and information corresponding to the location at which the radiation was delivered. The location at which the radiation was delivered may be recorded as coordinates or as one or more magnet current values, and the amount of the radiation that was delivered may be recorded as dosage in grays. Because the system is run open loop, the delivery of the radiation is not synchronized to the operation of the particle accelerator (e.g., to its RF cycle). However, the dosimetry may be synchronized to the operation of the particle accelerator. More specifically, the dosimetry records the amount and location of each dose delivered as the dose is delivered (that is, as close in time to delivery as possible given the limits of technology). Since the dose is delivered in synchronism with the operation of the accelerator (e.g., one pulse is delivered per RF cycle), in some implementations, the dosimetry that records the dose and the location operates in synchronism, or substantially in synchronism, with delivery of radiation doses to the target, and thus in synchronism with the operation of the particle accelerator, such as its RF cycle.

FIG. 14 shows a range modulator 115, which is an example implementation of energy degrader 110. In some implementations, such as that shown in FIG. 14 , the range modulator includes a series of plates 116. The plates may be made of one or more of the following example materials: carbon, beryllium or other material of low atomic number. Other materials, however, may be used in place of, or in addition to, these example materials.

One or more of the plates is movable into, or out of, the beam path to thereby affect the energy of the particle beam and, thus, the depth of penetration of the particle beam within the irradiation target. For example, the more plates that are moved into the path of the particle beam, the more energy that will be absorbed by the plates, and the less energy the particle beam will have. Conversely, the fewer plates that are moved into the path of the particle beam, the less energy that will be absorbed by the plates, and the more energy the particle beam will have. Higher energy particle beams typically penetrate deeper into the irradiation target than do lower energy particle beams. In this context, “higher” and “lower” are meant as relative terms, and do not have any specific numeric connotations.

Plates are moved physically into, and out of, the path of the particle beam. For example, as shown in FIG. 15 , a plate 116 a moves along the direction of arrow 117 between positions in the path of the particle beam and outside the path of the particle beam. The plates are computer-controlled. Generally, the number of plates that are moved into the path of the particle beam corresponds to the depth at which scanning of an irradiation target is to take place. For example, the irradiation target can be divided into cross-sections or depth-wise layers, each of which corresponds to an irradiation depth. One or more plates of the range modulator can be moved into, or out of, the beam path to the irradiation target in order to achieve the appropriate energy to irradiate each of these cross-sections or depth-wise layers of the irradiation target. The range modulator may be stationary relative to the particle beam during scanning of a part of (e.g., cross-section of) an irradiation target, except for its plates moving in and out of the path of the particle beam. Alternatively, the range modulator of FIGS. 14 and 15 may be replaced with a range modulator that, at least some of the time, tracks movement of the particle beam, thereby enabling use of smaller plates.

In implementations that use a range modulator of the type described above, the number of plates that are moved into the beam path determine/set the depth-wise layer of the irradiation target that is to be scanned. For example, if two plates are moved into the beam path, the layer will be more shallow than if one or no plates are moved into the beam path. The layer may be identified, and stored in memory, based on the number of plates moved into the beam path. In some implementations, the plates may have different heights. In such implementations, the heights of the various plates also affect which layer is to be scanned (e.g., how deep the particle beam will penetrate the target).

In some implementations, the particle accelerator may be a variable-energy particle accelerator. In example systems where a variable-energy particle accelerator is used, there may be less need for an energy degrader of the type described herein, as the energy level of the particle beam may be controlled by the particle accelerator. For example, in some systems that employ a variable-energy particle accelerator, an energy degrader may not be needed. In some systems that employ a variable-energy particle accelerator, an energy degrader may still be used to change beam energy levels.

In some implementations, a treatment plan is established prior to treating the irradiation target. The treatment plan may be stored in memory that is accessible to a computer system that controls operation of the particle therapy system. The treatment plan may include information about how radiation treatment is to be provided by the particle therapy system. For example, the treatment plan may specify how scanning is to be performed for a particular irradiation target. In some implementations, the treatment plan specifies that raster scanning is to be performed. Raster scanning includes producing an uninterrupted movement of the particle beam across the irradiation target. For example, the scanning magnet moves continually to scan (e.g., move) the particle beam across the irradiation target so as to produce uninterrupted movement of the particle beam over at least part of a layer of an irradiation target. The movement may be uninterrupted across an entire layer of the irradiation target or across only part of a layer. In some implementations, the beam may be moved at a constant speed along all or part of a layer of the irradiation target. In some implementations, the speed at which the beam is moved along all or part of a layer of the irradiation target may vary. For example, the particle beam may move more quickly across internal portions of a layer than at edges of the layer. The speed of movement may be specified in the treatment plan.

In some implementations, the treatment plan may also specify the target cumulative dose of radiation (particles) to be applied to various positions on layers of an irradiation target. The dose is cumulative in the sense that it may be achieved through application of one or more doses of particles. For example, the same location (e.g., in XYZ space) on an irradiation target may be irradiated ten times, each time with 10% of the target cumulative dose to achieve the target cumulative dose. In some implementations, the treatment plan need not specify the amount of dose for each location, the locations, or the number of times that locations are to be irradiated. That is, this information may be omitted from the treatment plan in some implementations. Rather, in some implementations, the intensity of the particle beam may be set beforehand to provide a particular dose of radiation per instance of irradiation. The particle beam may then be scanned over a layer of the irradiation target in an open loop manner, without requiring feedback to move to a next location. As the particle beam is scanned, the location of the beam is determined and the corresponding dose at that location is determined. The determination may be made at about the same time as the scanning and delivery (that is, as close in time to delivery as possible given the limits of technology). The cumulative dose at that location, which includes the current dose as well as any dose previously delivered during the current treatment, is compared to the target cumulative dose from the treatment plan. If the two do not match, then additional dose may be applied to that location during a subsequent scan. Since it is not always known precisely how much radiation will be delivered to a location per scan, the number of times that a location is scanned may not be set beforehand. Likewise, since there may be fluctuations in the amount of radiation actually delivered per scan to a location, the precise amount of radiation per scan is not necessarily set beforehand. Consequently, in some implementations, such information need not be included in the treatment plan.

In some implementations, the treatment plan may also include one or more patterns, over which the particle beam may be scanned per layer. The treatment plan may also specify the number of plates of an energy degrader to achieve a particular energy level/layer. Other implementations may include information in addition to, or instead of, that specified above.

In some implementations, the overall treatment plan of an irradiation target may include different treatment plans for different cross-sections (layers) of the irradiation target. The treatment plans for different cross-sections may contain the same information or different information, such as that provided above.

The scanning system includes the adaptive aperture of FIGS. 1 to 7, 30 , and 31 (or a variant thereof), which is placeable relative to the irradiation target to limit the extent of the particle beam and thereby limit the extent of the particle beam. For example, the adaptive aperture may be placed in the beam path down-beam of the energy degrader and before the particle beam hits the treatment area of the irradiation target. The adaptive aperture is controllable to allow the particle beam to pass therethrough and then hit certain parts of the treatment area, while preventing the particle beam from hitting other parts of the patient. For example, the adaptive aperture may be controlled to prevent the particle beam from hitting healthy tissue or to prevent the particle beam from hitting other parts of the irradiation target (e.g., if certain parts of the target are to receive more radiation than other parts). FIG. 16 depicts placement of an implementation 770 of the adaptive aperture described herein relative to a patient 771. The direction of beam 771 a is also shown.

As noted above, in some implementations, scanning is performed in an open-loop manner, e.g., by an open-loop control system that may be implemented using one or more processing devices, such as the computing device that controls the particle therapy system. In this example, open-loop scanning includes moving the particle beam across an irradiation target to substantially cover the target with radiation. In some implementations, movement is not synchronized with operation of the accelerator, e.g., with the RF frequency, but rather runs independently of the operation of the accelerator when the accelerator is operating. For example, movement of the particle beam may be uninterrupted, and not dependent upon the RF cycle of the particle accelerator. Uninterrupted movement may occur across all or part of a layer of an irradiation target. However, as described herein, the dosimetry may be synchronized with delivery of pulses of the particle beam to the irradiation target. In examples where the dosimetry is synchronized with delivery of pulses of the particle beam, the dosimetry is also synchronized with operation of the accelerator (e.g., with the RF frequency used to draw pulses of the particle beam from the ion source plasma column).

The radiation level of an individual dose of particle beam (e.g., an individual pulse from the accelerator) may be set beforehand. For example, each individual dose may be specified in grays. An individual dose may be, or correspond to, a percentage of the target cumulative dose that is to be applied to a location (e.g., an XYZ coordinate) in an irradiation target. In some implementations, the individual dose may be 100% of the target cumulative dose and, as a result, only a single scan may be needed to deliver a single dose of radiation (e.g., one or more particle pulses) per location to the irradiation target. In some implementations, the individual dose may be less than 100% of the target cumulative dose, resulting in the need for multiple scans of the same location to deliver multiple doses of radiation to the irradiation target. The individual dose may be any appropriate percentage of the target cumulative dose, such as: 1%, 2%, 3%, 4%, 5%, 6%, 7%, 8%, 9%, 10%, 11%, 12%, 13%, 14%, 15%, 16%, 17%, 18%, 19%, 20%, 25%, 30%, 35%, 40%, 45%, 50%, 55%, 60%, 65%, 70%, 75%, 80%, 85%, 90%, 95%, or any percentage in between these values.

The scanning magnet current may be controlled, in accordance with the treatment plan, to scan a depth-wise layer of the irradiation target. The layer is selected by appropriately positioning one or more energy degraders from the range compensator in the path of the particle beam and/or by setting an energy level of a variable-energy particle accelerator. As the layer is scanned, the current sensor samples the current applied to the scanning magnet. The amount of magnet current may be recorded, e.g., stored in memory. If more than one magnet or magnet coil is used, the amount of magnet current may be stored along with the identity of the magnet or coil. In addition, the current may be correlated to coordinates within the irradiation target (e.g., Cartesian XYZ coordinates) and those coordinates may be stored in addition to, or instead of, the corresponding magnet current. As explained above, the current sensor may sample the magnet current and correlate the sampling time to the time at which an irradiation dose (e.g., pulse) is delivered.

In this regard, ion chamber 109 may detect the intensity of doses delivered to the irradiation target as that dose is delivered. The intensity of each dose is recorded (e.g., stored in memory) along with the location of each delivered dose. As noted, the location of each delivered dose may be stored by coordinates, magnet current, or using some other appropriate metric. As noted above, the dosimetry—the dose verification—may be synchronized with delivery of the dose and, thus, with the output of the accelerator (which corresponds to the RF frequency, as described above). Accordingly, in some implementations, each time a dose is delivered, the intensity of that dose is determined almost immediately and the location at which the dose is applied is determined almost immediately. This information may be stored in one or more tables (e.g., one table per layer or multiple tables per layer) or other appropriate computer storage construct.

In some implementations, the tables may be updated as additional doses are delivered. For example, a table may keep a running track of the amount of dose delivered at each location. So, if the beam dose is “X” grays, at a first scan pass, the table may record X grays for a location. At a second scan pass, the table may record 2X grays, and so forth until the target cumulative dose is reached.

In this regard, for each location, a processing device associated with the accelerator (e.g., the computer system that controls the particle therapy system) may compare the cumulative dose from a table, such as that described above, to the target cumulative dose. If the cumulative dose matches the target cumulative dose, treatment for that location (or layer) is deemed completed. If the cumulative dose does not match the target cumulative dose, additional treatment is performed. For example, the layer or location is scanned again at the same locations, which are obtained from the table. The linear correlation between magnet current and beam movement produced by use of an air core magnet can facilitate repeated, and relatively accurate, repeated scanning at the same locations during multiple passes of the beam during scanning. The leaves of the adaptive aperture described herein may be moved slightly (e.g., a fraction of a millimeter, a millimeter, or multiple millimeters) between each scan of the same area, as described above.

Scanning may be repeated, at the same locations, any appropriate number of times until the target cumulative dose is reached at each location. In this regard, the entire layer may be re-scanned or only select portions of the layer may be re-scanned, dependent upon the target cumulative doses for the different locations on the layer. In some implementations, the intensity of the particle beam is not varied between scans. In other implementations, the intensity of the particle beam may be varied between scans, particularly if a small dose is required to top-off a cumulative dose to reach the target cumulative dose. The intensity of the dose may be increased or decreased, e.g., by altering the operation of the ion source (e.g., increasing the plasma ionization), altering the sweep of the RF frequency, or by any other appropriate methods.

As noted, scanning may be repeated for an entire layer or for only a portion of a layer. In some implementations, an entire layer, or a portion thereof, may be fully treated before treating another layer. That is, scanning may be repeated until the total cumulative dose is reached for each location on a layer before another layer is treated. In some implementations, each layer may be treated partially (e.g., scanned once) in sequence, and then re-scanned in sequence. In some implementations, several designated layers may be completely treated before other layers are treated. In some implementations, the entire target may be scanned once, followed by successive scans of the entire target until the appropriate total cumulative dose is delivered to each location.

During movement between layers, the beam may be turned-off. For example, during movement between layers, the ion source may be turned-off, thereby disrupting the output of the beam. During movement between layers, the RF sweep in the particle accelerator may be turned-off, thereby disrupting the extraction (and thus output) of the beam. During movement between layers, both the ion source and the circuitry that creates the RF sweep may be deactivated in some implementations. In some implementations, rather than turning-off the ion source and/or the RF sweep during movement between layers, the beam may be deflected to a beam-absorbing material using a kicker magnet (not shown) or the scanning magnet.

Different cross-sections of the irradiation target may be scanned according to different treatment plans. As described above, an energy degrader is used to control the scanning depth. In some implementations, the particle beam may be interrupted or redirected during configuration of the energy degrader. In other implementations, this need not be the case.

Described herein are examples of treating cross-sections of an irradiation target. These may be cross-sections that are roughly perpendicular to the direction of the particle beam. However, the concepts described herein are equally applicable to treating other portions of an irradiation target that are not cross-sections perpendicular to the direction of the particle beam. For example, an irradiation target may be segmented into spherical, cubical or other shaped volumes, and those volumes may be treated using the example processes, systems, and/or devices described herein.

FIG. 17 is a flowchart showing an example implementation of the scanning process described herein. Although process 200 of FIG. 17 is described in the context of the hardware described herein, process 200 may be performed using any appropriate hardware. The operations shown in process 200 may be performed in the same order as depicted or in a different order, where appropriate.

According to process 200, a treatment plan is stored (201). The treatment plan may be a treatment plan as described above. For example, the treatment plan may specify the type of scanning (e.g., uninterrupted raster scanning) and the total cumulative dose of radiation to be delivered to each location in each layer of an irradiation target. The treatment plan may omit, e.g., the doses to be delivered for each scan at individual locations and their intensities, as well as the number of doses to be delivered to each location and the identity of the locations.

An energy degrader may be set to select (202) a layer, and current may be applied to the magnet and controlled to move (203) the particle beam in accordance with a pattern set forth, e.g., in the treatment plan, to scan the layer. The current control may produce uninterrupted movement of the beam across at least part of the irradiation target to deliver doses of charged particles. An example of a pattern of beam movement 230 across a layer 233 of an irradiation target is shown in FIG. 18 . As the beam moves, each pulse of the beam delivers a dose of radiation to the target. The dose has an intensity, which may be set beforehand in the accelerator or during scanning, and is delivered to specific positions. The exact positions at which dose is to be delivered need not be set beforehand, but rather may be arrived at by a combination of beam movement and pulse output.

For positions at which the dose is delivered, information is stored (204) (or otherwise recorded), which identifies a location and an amount of dose delivered at the location. This information is typically stored after the dose is delivered. As explained above, the information may be determined as close to delivery of the dose as possible, using the ion chamber to determine particle beam intensity (e.g., the amount of the dose) and the current sensor on the scanning magnet to determine the location at which the dose is delivered. As described above, in some implementations, in synchronism with the delivery, information identifying doses of the particle beam delivered to the irradiation target is stored along with at least one of: coordinates at which the doses were delivered or magnet currents at which the doses were delivered. As also described above, this information may be stored in tables, which may be used to store the cumulative dose of radiation applied at positions on various layers of an irradiation target.

The entire layer may be scanned and information therefor recorded, as described above, or only part of the layer may be scanned and information therefor recorded. The adaptive aperture is mounted on an appropriate location of the scanning system in such as manner as to enable the adaptive aperture to track the particle beam's movement during scanning operations. At a point during scanning, the cumulative dose delivered at each position is compared to a target cumulative dose for that position. For example, this may be done after part of a layer containing that position is scanned, after the entire layer is scanned, after a set of layers are scanned, or after all layers in an irradiation target are scanned. It is determined (205) if the current cumulative dose matches the target cumulative dose at specific positions. If the current cumulative dose does match the target cumulative dose at specific positions, scanning is completed (207) for those positions. If the current cumulative dose does not match the target cumulative dose at specific positions, the scanning system is operated to compensate for deficiencies in the recorded (e.g., current cumulative) doses relative to corresponding target cumulative doses for those positions. For example, if the current cumulative dose does not match the target cumulative dose at specific positions, the current in the scanning magnet may be controlled in order to move (206) the beam so as to deliver additional dose to the specific positions.

As explained above, in some implementations, 100% of the dose may be applied during a single scan (e.g., a single delivery of particles) of a layer. In that case, more than one scan per layer may not be necessary. In other implementations, less than 100% of the dose may be applied during a single scan. In that case, more than one scan per layer will be necessary. To this end, according to the scanning process, for positions at which dose is applied, if the current cumulative dose at each position does not match the target cumulative dose at a corresponding position, the magnet current is controlled in order to move the beam so as to deliver additional dose to positions that require more dose. In other words, the layer may be re-scanned any appropriate number of times until the target cumulative dose is reached for all positions of the layer. In some implementations, in one scan or in multiple scans, the actual delivered dose may exceed 100% of the target cumulative dose. What dose to deliver may be dictated by appropriate medical professionals.

As noted above, the layer may be re-scanned at any appropriate point, e.g., after part of the layer is completed with a current scan, after the entire layer is completed with the current scan, after a set of layers is completed with a scan, or after all layers are completed with a scan. During re-scanning, the process above is repeated until the target cumulative dose is reached for all, or some subset of, positions in the irradiation target. In some implementations, the intensity of the particle beam may need to be adjusted, e.g., for the last scan. For example, if the intensity is set at 25% of the target cumulative dose, but only 20% is delivered at each scan, then a fifth (and possibly sixth) dose will require a lower intensity than 25% in order to reach the target cumulative dose.

The processes described herein may be used with a single particle accelerator, and any two or more of the features thereof described herein may be used with the single particle accelerator. The particle accelerator may be used in any type of medical or non-medical application. An example of a particle therapy system that may be used is provided below. Notably, the concepts described herein may be used in other systems not specifically described.

Referring to FIG. 19 , an example implementation of a charged particle radiation therapy system 400 includes a beam-producing particle accelerator 402 (e.g., the particle accelerator of FIGS. 8 and 9 ) having a weight and size small enough to permit it to be mounted on a rotating gantry 404 with its output directed straight (that is, essentially directly) from the accelerator housing toward a patient 406. Particle accelerator 402 also includes a scanning system of a type described herein (e.g., FIGS. 10 to 18 ).

In some implementations, the steel gantry has two

legs

408, 410 mounted for rotation on two

respective bearings

412, 414 that lie on opposite sides of the patient. The accelerator is supported by a steel truss 416 that is long enough to span a treatment area 418 in which the patient lies (e.g., twice as long as a tall person, to permit the person to be rotated fully within the space with any desired target area of the patient remaining in the line of the beam) and is attached stably at both ends to the rotating legs of the gantry.

In some examples, the rotation of the gantry is limited to a range 420 of less than 360 degrees, e.g., about 180 degrees, to permit a floor 422 to extend from a wall of the vault 424 that houses the therapy system into the patient treatment area. The limited rotation range of the gantry also reduces the required thickness of some of the walls (which are not directly aligned with the beam, e.g., wall 430), which provide radiation shielding of people outside the treatment area. A range of 180 degrees of gantry rotation is enough to cover all treatment approach angles, but providing a larger range of travel can be useful. For example the range of rotation may be between 180 and 330 degrees and still provide clearance for the therapy floor space. In other implementations, rotation is not limited as described above.

The horizontal rotational axis 432 of the gantry is located nominally one meter above the floor where the patient and therapist interact with the therapy system. This floor is positioned about 3 meters above the bottom floor of the therapy system shielded vault. The accelerator can swing under the raised floor for delivery of treatment beams from below the rotational axis. The patient couch moves and rotates in a substantially horizontal plane parallel to the rotational axis of the gantry. The couch can rotate through a range 434 of about 270 degrees in the horizontal plane with this configuration. This combination of gantry and patient rotational ranges and degrees of freedom allow the therapist to select virtually any approach angle for the beam. If needed, the patient can be placed on the couch in the opposite orientation and then all possible angles can be used.

In some implementations, the accelerator uses a synchrocyclotron configuration having a high magnetic field superconducting electromagnetic structure. Because the bend radius of a charged particle of a given kinetic energy is reduced in direct proportion to an increase in the magnetic field applied to it, the high magnetic field superconducting magnetic structure permits the accelerator to be made smaller and lighter. The synchrocyclotron uses a magnetic field that is uniform in rotation angle and falls off in strength with increasing radius. Such a field shape can be achieved regardless of the magnitude of the magnetic field, so in theory there is no upper limit to the magnetic field strength (and therefore the resulting particle energy at a fixed radius) that can be used in a synchrocyclotron.

The synchrocyclotron is supported on the gantry so that the beam is generated directly in line with the patient. The gantry permits rotation of the synchrocyclotron about a horizontal rotational axis that contains a point (isocenter 440) within, or near, the patient. The split truss that is parallel to the rotational axis, supports the synchrocyclotron on both sides.

Because the rotational range of the gantry is limited in some example implementations, a patient support area can be accommodated in a wide area around the isocenter. Because the floor can be extended broadly around the isocenter, a patient support table can be positioned to move relative to and to rotate about a vertical axis 442 through the isocenter so that, by a combination of gantry rotation and table motion and rotation, any angle of beam direction into any part of the patient can be achieved. In some implementations, the two gantry arms are separated by more than twice the height of a tall patient, allowing the couch with patient to rotate and translate in a horizontal plane above the raised floor.

Limiting the gantry rotation angle allows for a reduction in the thickness of at least one of the walls surrounding the treatment room. Thick walls, typically constructed of concrete, provide radiation protection to individuals outside the treatment room. A wall downstream of a stopping proton beam may be about twice as thick as a wall at the opposite end of the room to provide an equivalent level of protection. Limiting the range of gantry rotation enables the treatment room to be sited below earth grade on three sides, while allowing an occupied area adjacent to the thinnest wall reducing the cost of constructing the treatment room.

In the example implementation shown in FIG. 19 , the superconducting synchrocyclotron 402 operates with a peak magnetic field in a pole gap of the synchrocyclotron of 8.8 Tesla. The synchrocyclotron produces a beam of protons having an energy of 250 MeV. In some implementations, the synchrocyclotron is a variable-energy machine, and is capable of outputting proton beams having different energies. In some implementations, the synchrocyclotron may produce a beam having a fixed energy. In some implementations the field strength could be in the range of 4 T to 20 T and the proton energy could be in the range of 100 to 300 MeV.

The radiation therapy system described in this example is used for proton radiation therapy, but the same principles and details can be applied in analogous systems for use in heavy ion (ion) treatment systems.

As shown in FIGS. 8, 9, 20, 21, and 22 , an example synchrocyclotron 10 (e.g., 402 in FIG. 19 ) includes a magnet system 122 that contains a particle source 190, a radiofrequency drive system 191, and a beam extraction system. In this example, the magnetic field established by the magnet system has a shape appropriate to maintain focus of a contained proton beam using a combination of a split pair of annular

superconducting coils

140, 142 and a pair of shaped ferromagnetic (e.g., low carbon steel) pole faces 144, 146.

The two superconducting magnet coils are centered on a common axis and are spaced apart along the axis. The coils may be formed by of Nb₃Sn-based superconducting 0.8 mm diameter strands (that initially comprise a niobium-tin core surrounded by a copper sheath) deployed in a twisted cable-in-channel conductor geometry. After seven individual strands are cabled together, they are heated to cause a reaction that forms the final (brittle) superconducting material of the wire. After the material has been reacted, the wires are soldered into the copper channel (outer dimensions 3.18×2.54 mm and inner dimensions 2.08×2.08 mm) and covered with insulation (in this example, a woven fiberglass material). The copper channel containing the wires is then wound in a coil having a rectangular cross-section. The wound coil is then vacuum impregnated with an epoxy compound. The finished coils are mounted on an annular stainless steel reverse bobbin. Heater blankets may be placed at intervals in the layers of the windings to protect the assembly in the event of a magnet quench.

The entire coil can then be covered with copper sheets to provide thermal conductivity and mechanical stability and then contained in an additional layer of epoxy. The precompression of the coil can be provided by heating the stainless steel reverse bobbin and fitting the coils within the reverse bobbin. The reverse bobbin inner diameter is chosen so that when the entire mass is cooled to 4 K, the reverse bobbin stays in contact with the coil and provides some compression. Heating the stainless steel reverse bobbin to approximately 50 degrees C. and fitting coils at a temperature of 100 degrees Kelvin can achieve this.

The geometry of the coil is maintained by mounting the coils in a “reverse” rectangular bobbin to exert a restorative force that works against the distorting force produced when the coils are energized. As shown in FIG. 21 , in some implementations, coil position is maintained relative to corresponding magnet pole pieces and the cryostat using a set of warm-to-cold support straps 402, 404, 406. Supporting the cold mass with thin straps reduces the heat leakage imparted to the cold mass by the rigid support system. The straps are arranged to withstand the varying gravitational force on the coil as the magnet rotates on board the gantry. They withstand the combined effects of gravity and the large de-centering force realized by the coil when it is perturbed from a perfectly symmetric position relative to the magnet yoke. Additionally, the links act to reduce dynamic forces imparted on the coil as the gantry accelerates and decelerates when its position is changed. Each warm-to-cold support may include one S2 fiberglass link and one carbon fiber link. The carbon fiber link is supported across pins between the warm yoke and an intermediate temperature (50-70 K), and the S2 fiberglass link 408 is supported across the intermediate temperature pin and a pin attached to the cold mass. Each pin may be made of high strength stainless steel.

Referring to FIG. 8 , the field strength profile as a function of radius is determined largely by choice of coil geometry and pole face shape. The pole faces 144, 146 of the permeable yoke material can be contoured to fine tune the shape of the magnetic field to ensure that the particle beam remains focused during acceleration.

The superconducting coils are maintained at temperatures near absolute zero (e.g., about 4 degrees Kelvin) by enclosing the coil assembly (the coils and the bobbin) inside an evacuated annular aluminum or stainless steel cryostatic chamber 170 (the cryostat) that provides a free space around the coil structure, except at a limited set of support points 171, 173. In an alternate version (e.g., FIG. 9 ) the outer wall of the cryostat may be made of low carbon steel to provide an additional return flux path for the magnetic field.

In some implementations, the temperature near absolute zero is achieved and maintained using one single-stage Gifford-McMahon cryo-cooler and three two-stage Gifford McMahon cryo-coolers. Each two stage cryo-cooler has a second stage cold end attached to a condenser that recondenses Helium vapor into liquid Helium. In some implementations, the temperature near absolute zero is achieved and maintained using a cooling channel (not shown) containing liquid helium, which is formed inside a superconducting coil support structure (e.g., the reverse bobbin), and which contains a thermal connection between the liquid helium in the channel and the corresponding superconducting coil.

In some implementations, the coil assembly and cryostatic chambers are mounted within and fully enclosed by two

halves

181, 183 of a pillbox-shaped magnet yoke 100. The yoke 100 provides a path for the return magnetic field flux 184 and magnetically shields the volume 186 between the pole faces 144, 146 to prevent external magnetic influences from perturbing the shape of the magnetic field within that volume. The yoke also serves to decrease the stray magnetic field in the vicinity of the accelerator. In other implementations, the coil assembly and cryostatic chambers are mounted within and fully enclosed by a non-magnetic enclosure, and the path for return magnetic field flux is implemented using an active return system, an example of which is described above.

As shown in FIGS. 8 and 23 , the synchrocyclotron includes a particle source 190 of a Penning ion gauge geometry located near the geometric center 192 of the magnet structure. The particle source may be as described below.

Particle source

190 is fed from a supply 399 of hydrogen through a gas line 393 and tube 394 that delivers gaseous hydrogen. Electric cables 294 carry an electric current from a current source to stimulate electron discharge from cathodes 392, 390 that are aligned with the magnetic field.

In this example, the discharged electrons ionize the gas exiting through a small hole from tube 394 to create a supply of positive ions (protons) for acceleration by one semicircular (dee-shaped) radio-frequency plate that spans half of the space enclosed by the magnet structure and one dummy dee plate. In the case of an interrupted particle source, all (or a substantial part, e.g., a majority) of the tube containing plasma is removed at the acceleration region.

As shown in FIG. 24 , the dee plate 500 is a hollow metal structure that has two

semicircular surfaces

503, 505 that enclose a space 507 in which the protons are accelerated during half of their rotation around the space enclosed by the magnet structure. A duct 509 opening into the space 507 extends through the enclosure (e.g., the yoke or pole piece(s)) to an external location from which a vacuum pump can be attached to evacuate the space 507 and the rest of the space within a vacuum chamber in which the acceleration takes place. The dummy dee 502 comprises a rectangular metal ring that is spaced near to the exposed rim of the dee plate. The dummy dee is grounded to the vacuum chamber and magnet yoke. The dee plate 500 is driven by a radio-frequency signal that is applied at the end of a radio-frequency transmission line to impart an electric field in the space 507. The radio frequency electric field is made to vary in time as the accelerated particle beam increases in distance from the geometric center.

For the beam emerging from the centrally located particle source to clear the particle source structure as it begins to spiral outward, a large voltage difference may be applied across the radio frequency plates. 20,000 Volts is applied across the radio frequency plates. In some versions from 8,000 to 20,000 Volts may be applied across the radio frequency plates. To reduce the power required to drive this large voltage, the magnet structure is arranged to reduce the capacitance between the radio frequency plates and ground. This may be done by forming holes with sufficient clearance from the radio frequency structures through the outer yoke and the cryostat housing and making sufficient space between the magnet pole faces.

The high voltage alternating potential that drives the dee plate has a frequency that is swept downward during the accelerating cycle to account for the increasing relativistic mass of the protons and the decreasing magnetic field. The dummy dee does not require a hollow semi-cylindrical structure as it is at ground potential along with the vacuum chamber walls. Other plate arrangements could be used such as more than one pair of accelerating electrodes driven with different electrical phases or multiples of the fundamental frequency. The RF structure can be tuned to keep the Q high during the required frequency sweep by using, for example, a rotating capacitor having intermeshing rotating and stationary blades. During each meshing of the blades, the capacitance increases, thus lowering the resonant frequency of the RF structure. The blades can be shaped to create a precise frequency sweep required. A drive motor for the rotating condenser can be phase locked to the RF generator for precise control. One bunch of particles may be accelerated during each meshing of the blades of the rotating condenser.

The vacuum chamber in which the acceleration occurs is a generally cylindrical container that is thinner in the center and thicker at the rim. The vacuum chamber encloses the RF plates and the particle source and is evacuated by a vacuum pump. Maintaining a high vacuum reduces the chances that accelerating ions are not lost to collisions with gas molecules and enables the RF voltage to be kept at a higher level without arcing to ground.

Protons (or other ions) traverse a generally spiral orbital path beginning at the particle source. In half of each loop of the spiral path, the protons gain energy as they pass through the RF electric field. As the protons gain energy, the radius of the central orbit of each successive loop of their spiral path is larger than the prior loop until the loop radius reaches the maximum radius of the pole face. At that location a magnetic and electric field perturbation directs protons into an area where the magnetic field rapidly decreases, and the protons depart the area of the high magnetic field and are directed through an evacuated tube, referred to herein as the extraction channel, to exit the synchrocyclotron. A magnetic regenerator may be used to change the magnetic field perturbation to direct the protons. The protons exiting will tend to disperse as they enter an area of markedly decreased magnetic field that exists in the room around the synchrocyclotron.

Beam shaping elements

507, 509 in the extraction channel 138 (FIG. 21 ) redirect the protons so that they stay in a straight beam of limited spatial extent.

As the beam exits the extraction channel it is passed through a beam formation system 525 (FIG. 21 ), which may include a scanning system of the type described herein. Beam formation system 525 may be used in conjunction with an inner gantry that controls application of the beam.

Stray magnetic fields exiting from the synchrocyclotron may be limited by both a magnet yoke (which also serves as a shield) and a separate magnetic shield 514 (e.g., FIG. 8 ). The separate magnetic shield includes of a layer 517 of ferromagnetic material (e.g., steel or iron) that encloses the pillbox yoke, separated by a space 516. This configuration that includes a sandwich of a yoke, a space, and a shield achieves adequate shielding for a given leakage magnetic field at lower weight. As described above, in some implementations, an active return system may be used in place of, or to augment, the operation of the magnetic yoke and shield.

Referring to FIG. 19 , the gantry allows the synchrocyclotron to be rotated about a horizontal rotational axis 432. The truss structure 416 has two generally

parallel spans

480, 482. The synchrocyclotron is cradled between the spans about midway between the legs. The gantry is balanced for rotation about the

bearings using counterweights

622, 624 mounted on ends of the legs opposite the truss.

The gantry is driven to rotate by an electric motor mounted to one or both of the gantry legs and connected to the bearing housings by drive gears. The rotational position of the gantry is derived from signals provided by shaft angle encoders incorporated into the gantry drive motors and the drive gears.

At the location at which the ion beam exits the synchrocyclotron, the beam formation system 525 acts on the ion beam to give it properties suitable for patient treatment. For example, the beam may be spread and its depth of penetration varied to provide uniform radiation across a given target volume. The beam formation system may include active scanning elements as described herein.

All of the active systems of the synchrocyclotron (the current driven superconducting coils, the RF-driven plates, the vacuum pumps for the vacuum acceleration chamber and for the superconducting coil cooling chamber, the current driven particle source, the hydrogen gas source, and the RF plate coolers, for example), may be controlled by appropriate synchrocyclotron control electronics (not shown), which may include, e.g., one or more processing devices executing instructions from non-transitory memory to effect control.

As explained above, referring to system 602 of FIG. 25 , a beam-producing particle accelerator, in this case synchrocyclotron 604 (which may include any and all features described herein), may be mounted on rotating gantry 605. Rotating gantry 605 is of the type described herein, and can angularly rotate around patient support 606. This feature enables synchrocyclotron 604 to provide a particle beam essentially directly to the patient from various angles. For example, as in FIG. 25 , if synchrocyclotron 604 is above patient support 606, the particle beam may be directed downwards toward the patient. Alternatively, if synchrocyclotron 604 is below patient support 606, the particle beam may be directed upwards toward the patient. The particle beam is applied essentially directly to the patient in the sense that an intermediary beam routing mechanism is not required. A routing mechanism, in this context, is different from a shaping or sizing mechanism in that a shaping or sizing mechanism does not re-route the beam, but rather sizes and/or shapes the beam while maintaining the same general trajectory of the beam.

The particle accelerator used in the example particle therapy systems and example scanning systems described herein may be a variable-energy particle accelerator, an example of which is described below

The energy of an extracted particle beam (the particle beam output from the accelerator) can affect the use of the particle beam during treatment. In some machines, the energy of the particle beam (or particles in the particle beam) does not increase after extraction. However, the energy may be reduced based on treatment needs after the extraction and before the treatment. Referring to FIG. 26 , an example treatment system 910 includes an accelerator 912, e.g., a synchrocyclotron, from which a particle (e.g., proton) beam 914 having a variable energy is extracted to irradiate a target volume 924 of a body 922. Optionally, one or more additional devices, such as a scanning unit 916 or a scattering unit 916, one or more monitoring units 918, and an energy degrader 920, are placed along the irradiation direction 928. The devices intercept the cross-section of the extracted beam 914 and alter one or more properties of the extracted beam for the treatment.

A target volume to be irradiated (an irradiation target) by a particle beam for treatment typically has a three-dimensional configuration. In some examples, to carry-out the treatment, the target volume is divided into layers along the irradiation direction of the particle beam so that the irradiation can be done on a layer-by-layer basis. For certain types of particles, such as protons, the penetration depth (or which layer the beam reaches) within the target volume is largely determined by the energy of the particle beam. A particle beam of a given energy does not reach substantially beyond a corresponding penetration depth for that energy. To move the beam irradiation from one layer to another layer of the target volume, the energy of the particle beam is changed.

In the example shown in FIG. 26 , the target volume 924 is divided into nine layers 926 a-926 i along the irradiation direction 928. In an example process, the irradiation starts from the deepest layer 926 i, one layer at a time, gradually to the shallower layers and finishes with the shallowest layer 926 a. Before application to the body 922, the energy of the particle beam 914 is controlled to be at a level to allow the particle beam to stop at a desired layer, e.g., the layer 926 d, without substantially penetrating further into the body or the target volume, e.g., the layers 926 e-926 i or deeper into the body. In some examples, the desired energy of the particle beam 914 decreases as the treatment layer becomes shallower relative to the particle acceleration. In some examples, the beam energy difference for treating adjacent layers of the target volume 924 is about 3 MeV to about 100 MeV, e.g., about 10 MeV to about 80 MeV, although other differences may also be possible, depending on, e.g., the thickness of the layers and the properties of the beam.

The energy variation for treating different layers of the target volume 924 can be performed at the accelerator 912 (e.g., the accelerator can vary the energy) so that, in some implementations, no additional energy variation is required after the particle beam is extracted from the accelerator 912. So, the optional energy degrader 920 in the treatment system 10 may be eliminated from the system. In some implementations, the accelerator 912 can output particle beams having an energy that varies between about 100 MeV and about 300 MeV, e.g., between about 115 MeV and about 250 MeV. The variation can be continuous or non-continuous, e.g., one step at a time. In some implementations, the variation, continuous or non-continuous, can take place at a relatively high rate, e.g., up to about 50 MeV per second or up to about 20 MeV per second. Non-continuous variation can take place one step at a time with a step size of about 10 MeV to about 90 MeV.

When irradiation is complete in one layer, the accelerator 912 can vary the energy of the particle beam for irradiating a next layer, e.g., within several seconds or within less than one second. In some implementations, the treatment of the target volume 924 can be continued without substantial interruption or even without any interruption. In some situations, the step size of the non-continuous energy variation is selected to correspond to the energy difference needed for irradiating two adjacent layers of the target volume 924. For example, the step size can be the same as, or a fraction of, the energy difference.

In some implementations, the accelerator 912 and the degrader 920 collectively vary the energy of the beam 914. For example, the accelerator 912 provides a coarse adjustment and the degrader 920 provides a fine adjustment or vice versa. In this example, the accelerator 912 can output the particle beam that varies energy with a variation step of about 10-80 MeV, and the degrader 920 adjusts (e.g., reduces) the energy of the beam at a variation step of about 2-10 MeV.

The reduced use (or absence) of the energy degrader, such as a range modulator, may help to maintain properties and quality of the output beam from the accelerator, e.g., beam intensity. The control of the particle beam can be performed at the accelerator. Side effects, e.g., from neutrons generated when the particle beam passes the degrader 920 can be reduced or eliminated.

The energy of the particle beam 914 may be adjusted to treat another target volume 930 in another body or body part 922′ after completing treatment in target volume 924. The

target volumes

924, 930 may be in the same body (or patient), or in different patients. It is possible that the depth D of the target volume 930 from a surface of body 922′ is different from that of the target volume 924. Although some energy adjustment may be performed by the degrader 920, the degrader 912 may only reduce the beam energy and not increase the beam energy.

In this regard, in some cases, the beam energy required for treating target volume 930 is greater than the beam energy required to treat target volume 924. In such cases, the accelerator 912 may increase the output beam energy after treating the target volume 924 and before treating the target volume 930. In other cases, the beam energy required for treating target volume 930 is less than the beam energy required to treat target volume 924. Although the degrader 920 can reduce the energy, the accelerator 912 can be adjusted to output a lower beam energy to reduce or eliminate the use of the degrader 920. The division of the

target volumes

924, 930 into layers can be different or the same. The target volume 930 can be treated similarly on a layer by layer basis to the treatment of the target volume 924.

The treatment of the

different target volumes

924, 930 on the same patient may be substantially continuous, e.g., with the stop time between the two volumes being no longer than about 30 minutes or less, e.g., 25 minutes or less, 20 minutes or less, 15 minutes or less, 10 minutes or less, 5 minutes or less, or 1 minute or less. As explained herein, the accelerator 912 can be mounted on a movable gantry and the movement of the gantry can move the accelerator to aim at different target volumes. In some situations, the accelerator 912 can complete the energy adjustment of the output beam 914 during the time the treatment system makes adjustment (such as moving the gantry) after completing the treatment of the target volume 924 and before starting treating the target volume 930. After the alignment of the accelerator and the target volume 930, the treatment can begin with the adjusted, desired beam energy. Beam energy adjustment for different patients can also be completed relatively efficiently. In some examples, all adjustments, including increasing/reducing beam energy and/or moving the gantry are done within about 30 minutes, e.g., within about 25 minutes, within about 20 minutes, within about 15 minutes, within about 10 minutes or within about 5 minutes.

In the same layer of a target volume, an irradiation dose may be applied by moving the beam across the two-dimensional surface of the layer (which is sometimes called scanning beam) using a scanning unit 916. Alternatively, the layer can be irradiated by passing the extracted beam through one or more scatterers of the scattering unit 16 (which is sometimes called scattering beam).

Beam properties, such as energy and intensity, can be selected before a treatment or can be adjusted during the treatment by controlling the accelerator 912 and/or other devices, such as the scanning unit/scatterer(s) 916, the degrader 920, and others not shown in the figures. In example implementations, system 910 includes a controller 932, such as a computer, in communication with one or more devices in the system. Control can be based on results of the monitoring performed by the one or more monitors 918, e.g., monitoring of the beam intensity, dose, beam location in the target volume, etc. Although the monitors 918 are shown to be between the device 916 and the degrader 920, one or more monitors can be placed at other appropriate locations along the beam irradiation path. Controller 932 can also store a treatment plan for one or more target volumes (for the same patient and/or different patients). The treatment plan can be determined before the treatment starts and can include parameters, such as the shape of the target volume, the number of irradiation layers, the irradiation dose for each layer, the number of times each layer is irradiated, etc. The adjustment of a beam property within the system 910 can be performed based on the treatment plan. Additional adjustment can be made during the treatment, e.g., when deviation from the treatment plan is detected.

In some implementations, the accelerator 912 is configured to vary the energy of the output particle beam by varying the magnetic field in which the particle beam is accelerated. In an example implementation, one or more sets of coils receives variable electrical current to produce a variable magnetic field in the cavity. In some examples, one set of coils receives a fixed electrical current, while one or more other sets of coils receives a variable current so that the total current received by the coil sets varies. In some implementations, all sets of coils are superconducting. In other implementations, some sets of coils, such as the set for the fixed electrical current, are superconducting, while other sets of coils, such as the one or more sets for the variable current, are non-superconducting. In some examples, all sets of coils are non-superconducting.

Generally, the magnitude of the magnetic field is scalable with the magnitude of the electrical current. Adjusting the total electric current of the coils in a predetermined range can generate a magnetic field that varies in a corresponding, predetermined range. In some examples, a continuous adjustment of the electrical current can lead to a continuous variation of the magnetic field and a continuous variation of the output beam energy. Alternatively, when the electrical current applied to the coils is adjusted in a non-continuous, step-wise manner, the magnetic field and the output beam energy also varies accordingly in a non-continuous (step-wise) manner. The scaling of the magnetic field to the current can allow the variation of the beam energy to be carried out relatively precisely, although sometimes minor adjustment other than the input current may be performed.

In some implementations, to output particle beams having a variable energy, the accelerator 912 is configured to apply RF voltages that sweep over different ranges of frequencies, with each range corresponding to a different output beam energy. For example, if the accelerator 912 is configured to produce three different output beam energies, the RF voltage is capable of sweeping over three different ranges of frequencies. In another example, corresponding to continuous beam energy variations, the RF voltage sweeps over frequency ranges that continuously change. The different frequency ranges may have different lower frequency and/or upper frequency boundaries.

The extraction channel may be configured to accommodate the range of different energies produced by the variable-energy particle accelerator. For example the extraction channel may be large enough to support the highest and lowest energies produced by the particle accelerator. That is, the extraction channel may be sized or otherwise configured to receive and to transmit particles within that range of energies. Particle beams having different energies can be extracted from the accelerator 912 without altering the features of the regenerator that is used for extracting particle beams having a single energy. In other implementations, to accommodate the variable particle energy, the regenerator can be moved to disturb (e.g., change) different particle orbits in the manner described above and/or iron rods (magnetic shims) can be added or removed to change the magnetic field bump provided by the regenerator. More specifically, different particle energies will typically be at different particle orbits within the cavity. By moving the regenerator, it is possible to intercept a particle orbit at a specified energy and thereby provide the correct perturbation of that orbit so that particles at the specified energy reach the extraction channel. In some implementations, movement of the regenerator (and/or addition/removal of magnetic shims) is performed in real-time to match real-time changes in the particle beam energy output by the accelerator. In other implementations, particle energy is adjusted on a per-treatment basis, and movement of the regenerator (and/or addition/removal of magnetic shims) is performed in advance of the treatment. In either case, movement of the regenerator (and/or addition/removal of magnetic shims) may be computer controlled. For example, a computer may control one or more motors that effect movement of the regenerator and/or magnetic shims.

In some implementations, the regenerator is implemented using one or more magnetic shims that are controllable to move to the appropriate location(s).

As an example, table 1 shows three example energy levels at which example accelerator 912 can output particle beams. The corresponding parameters for producing the three energy levels are also listed. In this regard, the magnet current refers to the total electrical current applied to the one or more coil sets in the accelerator 912; the maximum and minimum frequencies define the ranges in which the RF voltage sweeps; and “r” is the radial distance of a location to a center of the cavity in which the particles are accelerated.

TABLE 1

Examples of beam energies and respective parameters.

Beam	Magnet	Maximum	Minimum	Magnetic Field	Magnetic Field
Energy	Current	Frequency	Frequency	at r = 0 mm	at r = 298 mm
(MeV)	(Amps)	(MHz)	(MHz)	(Tesla)	(Tesla)

250	1990	132	99	8.7	8.2
235	1920	128	97	8.4	8.0
211	1760	120	93	7.9	7.5

Details that may be included in an example particle accelerator that produces charged particles having variable energies are described below. The accelerator can be a synchrocyclotron and the particles may be protons. The particles may be output as pulsed beams. The energy of the beam output from the particle accelerator can be varied during the treatment of one target volume in a patient, or between treatments of different target volumes of the same patient or different patients. In some implementations, settings of the accelerator are changed to vary the beam energy when no beam (or particles) is output from the accelerator. The energy variation can be continuous or non-continuous over a desired range.

Referring to the example shown in FIG. 8 , the particle accelerator, which may be a variable-energy particle accelerator like accelerator 912 described above, may be configured to output particle beams that have a variable energy. The range of the variable energy can have an upper boundary that is about 200 MeV to about 300 MeV or higher, e.g., 200 MeV, about 205 MeV, about 210 MeV, about 215 MeV, about 220 MeV, about 225 MeV, about 230 MeV, about 235 MeV, about 240 MeV, about 245 MeV, about 250 MeV, about 255 MeV, about 260 MeV, about 265 MeV, about 270 MeV, about 275 MeV, about 280 MeV, about 285 MeV, about 290 MeV, about 295 MeV, or about 300 MeV or higher. The range can also have a lower boundary that is about 100 MeV or lower to about 200 MeV, e.g., about 100 MeV or lower, about 105 MeV, about 110 MeV, about 115 MeV, about 120 MeV, about 125 MeV, about 130 MeV, about 135 MeV, about 140 MeV, about 145 MeV, about 150 MeV, about 155 MeV, about 160 MeV, about 165 MeV, about 170 MeV, about 175 MeV, about 180 MeV, about 185 MeV, about 190 MeV, about 195 MeV, about 200 MeV.

In some examples, the variation is non-continuous and the variation step can have a size of about 10 MeV or lower, about 15 MeV, about 20 MeV, about 25 MeV, about 30 MeV, about 35 MeV, about 40 MeV, about 45 MeV, about 50 MeV, about 55 MeV, about 60 MeV, about 65 MeV, about 70 MeV, about 75 MeV, or about 80 MeV or higher. Varying the energy by one step size can take no more than 30 minutes, e.g., about 25 minutes or less, about 20 minutes or less, about 15 minutes or less, about 10 minutes or less, about 5 minutes or less, about 1 minute or less, or about 30 seconds or less. In other examples, the variation is continuous and the accelerator can adjust the energy of the particle beam at a relatively high rate, e.g., up to about 50 MeV per second, up to about 45 MeV per second, up to about 40 MeV per second, up to about 35 MeV per second, up to about 30 MeV per second, up to about 25 MeV per second, up to about 20 MeV per second, up to about 15 MeV per second, or up to about 10 MeV per second. The accelerator can be configured to adjust the particle energy both continuously and non-continuously. For example, a combination of the continuous and non-continuous variation can be used in a treatment of one target volume or in treatments of different target volumes. Flexible treatment planning and flexible treatment can be achieved.

A particle accelerator that outputs a particle beam having a variable energy can provide accuracy in irradiation treatment and reduce the number of additional devices (other than the accelerator) used for the treatment. For example, the use of degraders for changing the energy of an output particle beam may be reduced or eliminated for all or part of the treatment. The properties of the particle beam, such as intensity, focus, etc. can be controlled at the particle accelerator and the particle beam can reach the target volume without substantial disturbance from the additional devices. The relatively high variation rate of the beam energy can reduce treatment time and allow for efficient use of the treatment system.

In some implementations, the accelerator, such as the synchrocyclotron of FIG. 8 , accelerates particles or particle beams to variable energy levels by varying the magnetic field in the accelerator, which can be achieved by varying the electrical current applied to coils for generating the magnetic field. As explained above, an example synchrocyclotron (e.g., the synchrocyclotron of FIG. 8 ) includes a magnet system that contains a particle source, a radiofrequency drive system, and a beam extraction system. FIG. 27 shows an example of a magnet system that may be used in a variable-energy accelerator. In this example implementation, the magnetic field established by the magnet system 1012 can vary by about 5% to about 35% of a maximum value of the magnetic field that two sets of

coils

40 a and 40 b, and 42 a and 42 b are capable of generating. The magnetic field established by the magnet system has a shape appropriate to maintain focus of a contained proton beam using a combination of the two sets of coils and a pair of shaped ferromagnetic (e.g., low carbon steel) structures, examples of which are provided above.

Each set of coils may be a split pair of annular coils to receive electrical current. In some situations, both sets of coils are superconducting. In other situations, only one set of the coils is superconducting and the other set is non-superconducting or normal conducting (also discussed further below). It is also possible that both sets of coils are non-superconducting. Suitable superconducting materials for use in the coils include niobium-3 tin (Nb₃Sn) and/or niobium-titanium. Other normal conducting materials can include copper. Examples of the coil set constructions are described further below.

The two sets of coils can be electrically connected serially or in parallel. In some implementations, the total electrical current received by the two sets of coils can include about 2 million ampere turns to about 10 million ampere turns, e.g., about 2.5 to about 7.5 million ampere turns or about 3.75 million ampere turns to about 5 million ampere turns. In some examples, one set of coils is configured to receive a fixed (or constant) portion of the total variable electrical current, while the other set of coils is configured to receive a variable portion of the total electrical current. The total electrical current of the two coil sets varies with the variation of the current in one coil set. In other situations, the electrical current applied to both sets of coils can vary. The variable total current in the two sets of coils can generate a magnetic field having a variable magnitude, which in turn varies the acceleration pathways of the particles and produces particles having variable energies.

Generally, the magnitude of the magnetic field generated by the coil(s) is scalable to the magnitude of the total electrical current applied to the coil(s). Based on the scalability, in some implementations, linear variation of the magnetic field strength can be achieved by linearly changing the total current of the coil sets. The total current can be adjusted at a relatively high rate that leads to a relatively high-rate adjustment of the magnetic field and the beam energy.

In the example reflected in Table 1 above, the ratio between values of the current and the magnetic field at the geometric center of the coil rings is: 1990:8.7 (approximately 228.7:1); 1920:8.4 (approximately 228.6:1); 1760:7.9 (approximately 222.8:1). Accordingly, adjusting the magnitude of the total current applied to a superconducting coil(s) can proportionally (based on the ratio) adjust the magnitude of the magnetic field.

The scalability of the magnetic field to the total electrical current in the example of Table 1 is also shown in the plot of FIG. 28 , where BZ is the magnetic field along the Z direction; and R is the radial distance measured from a geometric center of the coil rings along a direction perpendicular to the Z direction. The magnetic field has the highest value at the geometric center, and decreases as the distance R increases. The curves 1035, 1037 represent the magnetic field generated by the same coil sets receiving different total electrical current: 1760 Amperes and 1990 Amperes, respectively. The corresponding energies of the extracted particles are 211 MeV and 250 MeV, respectively. The two curves 1035, 1037 have substantially the same shape and the different parts of the curves 1035, 1037 are substantially parallel. As a result, either the curve 1035 or the curve 1037 can be linearly shifted to substantially match the other curve, indicating that the magnetic field is scalable to the total electrical current applied to the coil sets.

In some implementations, the scalability of the magnetic field to the total electrical current may not be perfect. For example, the ratio between the magnetic field and the current calculated based on the example shown in table 1 is not constant. Also, as shown in FIG. 28 , the linear shift of one curve may not perfectly match the other curve. In some implementations, the total current is applied to the coil sets under the assumption of perfect scalability. The target magnetic field (under the assumption of perfect scalability) can be generated by additionally altering the features, e.g., geometry, of the coils to counteract the imperfection in the scalability. As one example, ferromagnetic (e.g., iron) rods (magnetic shims) can be inserted or removed from one or both of the magnetic structures (e.g., yokes, pole pieces, and the like). The features of the coils can be altered at a relatively high rate so that the rate of the magnetic field adjustment is not substantially affected as compared to the situation in which the scalability is perfect and only the electrical current needs to be adjusted. In the example of iron rods, the rods can be added or removed at the time scale of seconds or minutes, e.g., within 5 minutes, within 1 minute, less than 30 seconds, or less than 1 second.

In some implementations, settings of the accelerator, such as the current applied to the coil sets, can be chosen based on the substantial scalability of the magnetic field to the total electrical current in the coil sets.

Generally, to produce the total current that varies within a desired range, any appropriate combination of current applied to the two coil sets can be used. In an example, the coil set 42 a, 42 b can be configured to receive a fixed electrical current corresponding to a lower boundary of a desired range of the magnetic field. In the example shown in table 1, the fixed electrical current is 1760 Amperes. In addition, the coil set 40 a, 40 b can be configured to receive a variable electrical current having an upper boundary corresponding to a difference between an upper boundary and a lower boundary of the desired range of the magnetic field. In the example shown in table 1, the coil set 40 a, 40 b is configured to receive electrical current that varies between 0 Ampere and 230 Amperes.

In another example, the coil set 42 a, 42 b can be configured to receive a fixed electrical current corresponding to an upper boundary of a desired range of the magnetic field. In the example shown in table 1, the fixed current is 1990 Amperes. In addition, the coil set 40 a, 40 b can be configured to receive a variable electrical current having an upper boundary corresponding to a difference between a lower boundary and an upper boundary of the desired range of the magnetic field. In the example shown in table 1, the coil set 40 a, 40 b is configured to receive electrical current that varies between −230 Ampere and 0 Ampere.

The total variable magnetic field generated by the variable total current for accelerating the particles can have a maximum magnitude greater than 4 Tesla, e.g., greater than 5 Tesla, greater than 6 Tesla, greater than 7 Tesla, greater than 8 Tesla, greater than 9 Tesla, or greater than 10 Tesla, and up to about 20 Tesla or higher, e.g., up to about 18 Tesla, up to about 15 Tesla, or up to about 12 Tesla. In some implementations, variation of the total current in the coil sets can vary the magnetic field by about 0.2 Tesla to about 4.2 Tesla or more, e.g., about 0.2 Tesla to about 1.4 Tesla or about 0.6 Tesla to about 4.2 Tesla. In some situations, the amount of variation of the magnetic field can be proportional to the maximum magnitude.

FIG. 29 shows an example RF structure for sweeping the voltage on the dee plate 500 over an RF frequency range for each energy level of the particle beam, and for varying the frequency range when the particle beam energy is varied. The

semicircular surfaces

503, 505 of the dee plate 500 are connected to an inner conductor 1300 and housed in an outer conductor 1302. The high voltage is applied to the dee plate 500 from a power source (not shown, e.g., an oscillating voltage input) through a power coupling device 1304 that couples the power source to the inner conductor. In some implementations, the coupling device 1304 is positioned on the inner conductor 1300 to provide power transfer from the power source to the dee plate 500. In addition, the dee plate 500 is coupled to variable

reactive elements

1306, 1308 to perform the RF frequency sweep for each particle energy level, and to change the RF frequency range for different particle energy levels.

The variable reactive element 1306 can be a rotating capacitor that has multiple blades 1310 rotatable by a motor (not shown). By meshing or unmeshing the blades 1310 during each cycle of RF sweeping, the capacitance of the RF structure changes, which in turn changes the resonant frequency of the RF structure. In some implementations, during each quarter cycle of the motor, the blades 1310 mesh with the each other. The capacitance of the RF structure increases and the resonant frequency decreases. The process reverses as the blades 1310 unmesh. As a result, the power required to generate the high voltage applied to the dee plate 103 and necessary to accelerate the beam can be reduced by a large factor. In some implementations, the shape of the blades 1310 is machined to form the required dependence of resonant frequency on time.

The RF frequency generation is synchronized with the blade rotation by sensing the phase of the RF voltage in the resonator, keeping the alternating voltage on the dee plates close to the resonant frequency of the RF cavity. (The dummy dee is grounded and is not shown in FIG. 29 ).

The variable reactive element 1308 can be a capacitor formed by a plate 1312 and a surface 1316 of the inner conductor 1300. The plate 1312 is movable along a direction 1314 towards or away from the surface 1316. The capacitance of the capacitor changes as the distance D between the plate 1312 and the surface 1316 changes. For each frequency range to be swept for one particle energy, the distance D is at a set value, and to change the frequency range, the plate 1312 is moved corresponding to the change in the energy of the output beam.

In some implementations, the inner and

outer conductors

1300, 1302 are formed of a metallic material, such as copper, aluminum, or silver. The blades 1310 and the plate 1312 can also be formed of the same or different metallic materials as the

conductors

1300, 1302. The coupling device 1304 can be an electrical conductor. The variable

reactive elements

1306, 1308 can have other forms and can couple to the dee plate 100 in other ways to perform the RF frequency sweep and the frequency range alteration. In some implementations, a single variable reactive element can be configured to perform the functions of both the variable

reactive elements

1306, 1308. In other implementations, more than two variable reactive elements can be used.

The control of the gantry, the patient support, the active beam shaping elements, and the synchrocyclotron to perform a therapy session is achieved by appropriate therapy control electronics (not shown).

Control of the particle therapy system described herein and its various features may be implemented using hardware or a combination of hardware and software. For example, a system like the ones described herein may include various controllers and/or processing devices located at various points. A central computer may coordinate operation among the various controllers or processing devices. The central computer, controllers, and processing devices may execute various software routines to effect control and coordination of testing and calibration.

System operation can be controlled, at least in part, using one or more computer program products, e.g., one or more computer program tangibly embodied in one or more non-transitory machine-readable media, for execution by, or to control the operation of, one or more data processing apparatus, e.g., a programmable processor, a computer, multiple computers, and/or programmable logic components.

A computer program can be written in any form of programming language, including compiled or interpreted languages, and it can be deployed in any form, including as a stand-alone program or as a module, component, subroutine, or other unit suitable for use in a computing environment. A computer program can be deployed to be executed on one computer or on multiple computers at one site or distributed across multiple sites and interconnected by a network.

Actions associated with implementing all or part of the operations of the particle therapy system described herein can be performed by one or more programmable processors executing one or more computer programs to perform the functions described herein. All or part of the operations can be implemented using special purpose logic circuitry, e.g., an FPGA (field programmable gate array) and/or an ASIC (application-specific integrated circuit).

Processors suitable for the execution of a computer program include, by way of example, both general and special purpose microprocessors, and any one or more processors of any kind of digital computer. Generally, a processor will receive instructions and data from a read-only storage area or a random access storage area or both. Elements of a computer (including a server) include one or more processors for executing instructions and one or more storage area devices for storing instructions and data. Generally, a computer will also include, or be operatively coupled to receive data from, or transfer data to, or both, one or more machine-readable storage media, such as mass PCBs for storing data, e.g., magnetic, magneto-optical disks, or optical disks. Non-transitory machine-readable storage media suitable for embodying computer program instructions and data include all forms of non-volatile storage area, including by way of example, semiconductor storage area devices, e.g., EPROM, EEPROM, and flash storage area devices; magnetic disks, e.g., internal hard disks or removable disks; magneto-optical disks; and CD-ROM and DVD-ROM disks.

Any “electrical connection” as used herein may imply a direct physical connection or a wired or wireless connection that includes intervening components but that nevertheless allows electrical signals to flow between connected components. Any “connection” involving electrical circuitry mentioned herein, unless stated otherwise, is an electrical connection and not necessarily a direct physical connection regardless of whether the word “electrical” is used to modify “connection”.

Any two more of the foregoing implementations may be used in an appropriate combination in an appropriate particle accelerator (e.g., a synchrocyclotron). Likewise, individual features of any two more of the foregoing implementations may be used in an appropriate combination.

Elements of different implementations described herein may be combined to form other implementations not specifically set forth above. Elements may be left out of the processes, systems, apparatus, etc., described herein without adversely affecting their operation. Various separate elements may be combined into one or more individual elements to perform the functions described herein.

The example implementations described herein are not limited to use with a particle therapy system or to use with the example particle therapy systems described herein. Rather, the example implementations can be used in any appropriate system that directs accelerated particles to an output.

Other implementations not specifically described herein are also within the scope of the following claims.

Claims

What is claimed is:

1. A device to trim a particle beam, the device comprising:

a carrier configured to move in a direction into a field that is scanned by the particle beam, the field having two dimensions, the carrier comprising multiple leaves comprised of material to block passage of the particle beam, the multiple leaves being arranged on the carrier to move along with the carrier and being configured to move outward from the carrier in the direction and further into the field, the multiple leaves together defining an edge that is movable into a path of the particle beam such that a first part of the particle beam on a first side of the edge is blocked by the multiple leaves and such that a second part of the particle beam on a second side of the edge is not blocked by the multiple leaves, the multiple leaves being controllable to configure the edge to trim a single spot defined by a cross-section of the particle beam, and the multiple leaves being controllable to configure the edge to trim an area to be covered by multiple spots of the particle beam, the multiple leaves being individually and collectively smaller than the field in each of the two dimensions.

2. The device of claim 1, wherein the carrier is a first carrier, the direction is a first direction, the multiple leaves are first multiple leaves, and the edge is a first edge; and

wherein the device comprises a second carrier configured to move in a second direction into the field that is scanned by the particle beam, the second carrier comprising second multiple leaves comprised of material to block passage of the particle beam, the second multiple leaves being arranged on the second carrier to move along with the second carrier and being configured to move outward from the second carrier in the second direction and further into the field, the second multiple leaves together defining a second edge that is movable into the path of the particle beam such that a third part of the particle beam on a first side of the second edge is blocked by the second multiple leaves and such that the second part of the particle beam on a second side of the second edge is not blocked by the second multiple leaves, the second multiple leaves being controllable to configure the second edge to trim the single spot defined by the cross-section of the particle beam, and the second multiple leaves being controllable to configure the second edge to trim the area to be covered by the multiple spots of the particle beam.

3. The device of claim 2, wherein the first edge and the second edge comprise edges of a single aperture through which the second part of the particle beam is passable, with the first edge and the second edge collimating at least part of the particle beam.

4. The device of claim 3, wherein the first multiple leaves are configurable so that the first edge has an irregular shape, and the second multiple leaves are configurable so that the second edge has an irregular shape, the first edge and the second edge mimicking a machined patient-specific aperture.

5. The device of claim 2, wherein the first multiple leaves are controllable to configure the first edge differently for different depth-wise layers of an irradiation target to be treated by the particle beam, and the second multiple leaves are controllable to configure the second edge differently for different depth-wise layers of the irradiation target to be treated by the particle beam.

6. The device of claim 3, wherein the first direction and the second direction are in a first dimension of a coordinate system; and

wherein the device comprises a track to which the first carrier and the second carrier are coupled, the first carrier and the second carrier being movable along the track in a second dimension of the coordinate system, the second dimension being different than the first dimension.

7. The device of claim 6, wherein the first carrier and the second carrier are movable in concert along the track.

8. The device of claim 6, wherein the first carrier and the second carrier are movable independently along the track.

9. The device of claim 1, wherein the multiple leaves comprise ends that face the field, each of the ends being flat.

10. The device of claim 1, wherein the multiple leaves comprise ends least partly face the field, each of the ends being at least partly curved.

11. A particle therapy system comprising:

a particle accelerator to generate a particle beam;

one or more scanning magnets to scan the particle beam relative to an irradiation target in a patient; and

a device to trim the particle beam so that at least part of a spot of the particle beam reaches the irradiation target, the device being between the one or more scanning magnets and the patient, the device comprising:

a carrier configured to move in a direction into a field that is scanned by the particle beam, the field having two dimensions, the carrier comprising multiple leaves comprised of material to block passage of the particle beam, the multiple leaves being arranged on the carrier to move along with the carrier and being configured to move outward from the carrier in the direction and further into the field, the multiple leaves together defining an edge that is movable into a path of the particle beam such that a first part of the particle beam on a first side of the edge is blocked from reaching the patient by the multiple leaves and such that a second part of the particle beam on a second side of the edge is not blocked by the multiple leaves and reaches the irradiation target, the multiple leaves being controllable to define the edge based on a size of the spot independent of other spots of the particle beam, the multiple leaves being individually and collectively smaller than the field in each of the two dimensions.

12. The particle therapy system of claim 11, further comprising:

a control system to receive information defining a size of the spot, the control system using the information to configure the multiple leaves to define the edge to trim the spot.

13. The particle therapy system of claim 11, wherein the particle accelerator is a synchrocyclotron; and

wherein the particle therapy system further comprises a gantry on which at least the synchrocyclotron is mounted, the gantry being rotatable around at least part of a patient to position the particle beam.

14. The particle therapy system of claim 13; wherein the synchrocyclotron comprises:

a voltage source to provide a radio frequency (RF) voltage to a cavity to accelerate particles from a particle source, the voltage source being configured to sweep the RF voltage over a frequency range in a cycle;

a coil to receive electrical current having one of multiple values and to generate a magnetic field corresponding to the electrical current, the magnetic field for causing the particles to move orbitally within the cavity at an energy that corresponds to the electrical current; the magnetic field being at least 4 Tesla; and

an extraction channel to receive the particles from the cavity and to output the particles received from the cavity to the one or more scanning magnets, the particles that are output from the cavity having an energy that corresponds to the electrical current;

wherein the energy of the particles that are output from the cavity is variable in a range that is between about 100 MeV and about 300 MeV.

15. The particle therapy system of claim 11, wherein the carrier is a first carrier, the direction is a first direction, the multiple leaves are first multiple leaves, and the edge is a first edge; and

wherein the device comprises a second carrier configured to move in a second direction into the field that is scanned by the particle beam, the second carrier comprising second multiple leaves comprised of material to block passage of the particle beam, the second multiple leaves being arranged on the second caner to move along with the second carrier and being configured to move outward from the second carrier in the second direction and further into the field, the second multiple leaves together defining a second edge that is movable into the path of the particle beam such that a third part of the particle beam on a first side of the second edge is blocked by the second multiple leaves and such that the second part of the particle beam on a second side of the second edge is not blocked by the second multiple leaves, the second multiple leaves being controllable to define the second edge based on the size of the spot independent of the other spots of the particle beam.

16. The particle therapy system of claim 15, wherein the first edge and the second edge comprise edges of a single aperture through which the second part of the particle beam is passable, with the first edge and the second edge collimating at least part of the particle beam.

17. The particle therapy system of claim 15, wherein the first multiple leaves are configurable so that the first edge has an irregular shape, and the second multiple leaves are configurable so that the second edge has an irregular shape, the first edge and the second edge mimicking a machined patient-specific aperture.

18. The particle therapy system of claim 15, wherein the first multiple leaves are controllable to configure the first edge differently for different depth-wise layers of the irradiation target, and the second multiple leaves are controllable to configure the second edge differently for different depth-wise layers of the irradiation target.

19. The particle therapy system of claim 15, wherein the first direction and the second direction are in a first dimension of a coordinate system; and

20. A device to trim a particle beam, the device comprising:

a carrier configured to move in a direction into a field that is scanned by the particle beam, the field having two dimensions, the carrier comprising multiple leaves comprised of material to block passage of the particle beam, the multiple leaves being arranged on the carrier to move along with the carrier and being configured to move outward from the carrier in the direction and further into the field, the multiple leaves together defining an edge that is movable into a path of the particle beam such that a first part of the particle beam on a first side of the edge is blocked by the multiple leaves and such that a second part of the particle beam on a second side of the edge is not blocked by the multiple leaves, the multiple leaves being controllable to configure the edge to trim a single spot defined by a cross-section of the particle beam by blocking the first part of the particle beam, the multiple leaves being controllable to configure the edge to perform trimming on an individual spot-by-spot basis during scanning by the particle beam, the multiple leaves being individually and collectively smaller than the field in each of the two dimensions.